From jankner at anl.gov  Thu Jan 20 22:05:21 2000
From: jankner at anl.gov (Ankner, John)
Date: Thu, 20 Jan 2000 15:05:21 -0600
Subject: Windows compilation
Message-ID: <A0E27DD848C1D211AE10006097C9C0BB05881E@exchmail.pns.anl.gov>

Having looked at the messages in the mailing list archive, I am unable to
determine what steps are required to compile the mcstas distribution using
Visual C++ on a Windows NT box.  In particular, there are a lot of files of
unknown provenance in the unpacked mcstas-1.17A4 directory and I don't know
which to transfer to my NT directory.  In addition, I am not clear on the
redefinition of the WIN32 macro -- to what should I redefine it?  Anybody
who can answer these relatively trivial questions would earn my undying
devotion.
JFA


From kristian.nielsen at risoe.dk  Fri Jan 21 09:03:06 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: Fri, 21 Jan 2000 09:03:06 +0100
Subject: Windows compilation
In-Reply-To: <A0E27DD848C1D211AE10006097C9C0BB05881E@exchmail.pns.anl.gov>
 (jankner@anl.gov)
Message-ID: <01JKYLOBCWCA914Q0P@risoe.dk>

> Date: Thu, 20 Jan 2000 15:05:21 -0600
> From: "Ankner, John" <jankner at anl.gov>

> Having looked at the messages in the mailing list archive, I am unable to
> determine what steps are required to compile the mcstas distribution using
> Visual C++ on a Windows NT box.  In particular, there are a lot of files of
> unknown provenance in the unpacked mcstas-1.17A4 directory and I don't know
> which to transfer to my NT directory.  In addition, I am not clear on the
> redefinition of the WIN32 macro -- to what should I redefine it?  Anybody

Just copy all of the files ending in ".c" and ".h". Then ask your
compiler to compile all the ".c" files into a 32-bit console
application called "mcstas.exe".

You should also copy the "lib" subdirectory to C:\mcstas\lib on the
Windows machine (you can copy it to some other directory if you define
the C preprocessor macro MC_SYS_DIR to be the directory name as a
string).

The definition of WIN32 can be anything, the usual convention is to set
it to the number 1. I think there is some menu entry somewhere in Visual
C++ to set it, otherwise you could probably put the line

#define WIN32 1

at the top of the file "port.h".

If you get problems compiling the C files generated by McStas, try using
the "--portable" flag on the mcstas compiler. Or even better, tell me
how to create a new directory in Visual C++ (this is the only thing in
the generated simulations that is not pure ANSI C).

I am happy that someone is once again looking into compiling McStas on
Windows. If your compiler is unhelpful and spits out nasty error
messages, send them in an email and I will try to sort things out.

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790



From rotter at physik.tu-dresden.de  Mon Jan 31 16:10:04 2000
From: rotter at physik.tu-dresden.de (martin rotter)
Date: Mon, 31 Jan 2000 16:10:04 +0100
Subject: pgperl problem
Message-ID: <3895A5CC.17E805BE@physik.tu-dresden.de>

I was not able to install the PgPerl 2.15 library
on linux suse 6.2

Please find enclosed an error report.

PGPLOT compiles successfully, however
make test gives the output shown in file o4
(o1, o2, o3 conatin the output of Perl -V,
perl Makefile.PL, make - respectively)


The problem seems to be that the /usr/local/pgplot/libpgplot.so is not
compatible with blib/arch/auto/PGPLOT.so


I would appreciate any help on this problem
because I not very expierenced (I have managed
to run PgPerl under Suse 6.0 system, files *ok
contain the description of this system)

With best regards
Martin R

I. LINUX SUSE 6.2 INSTALLATION CONFIGURATION WITH PROBLEMS:

Summary of my perl5 (5.0 patchlevel 5 subversion 3) configuration:
  Platform:
    osname=linux, osvers=2.2.10, archname=i586-linux
    uname='linux fatou 2.2.10 #2 smp thu jul 15 15:03:02 mest 1999 i686 unknown
'
    hint=recommended, useposix=true, d_sigaction=define
    usethreads=undef useperlio=undef d_sfio=undef
  Compiler:
    cc='cc', optimize='-O2 -pipe', gccversion=egcs-2.91.66 19990314/Linux
(egcs-1.1.2 release)
    cppflags='-Dbool=char -DHAS_BOOL -I/usr/local/include'
    ccflags ='-Dbool=char -DHAS_BOOL -I/usr/local/include'
    stdchar='char', d_stdstdio=undef, usevfork=false
    intsize=4, longsize=4, ptrsize=4, doublesize=8
    d_longlong=define, longlongsize=8, d_longdbl=define, longdblsize=12
    alignbytes=4, usemymalloc=n, prototype=define
  Linker and Libraries:
    ld='cc', ldflags =' -L/usr/local/lib'
    libpth=/usr/local/lib /lib /usr/lib
    libs=-lnsl -lndbm -lgdbm -ldb -ldl -lm -lc -lposix -lcrypt
    libc=, so=so, useshrplib=false, libperl=libperl.a
  Dynamic Linking:
    dlsrc=dl_dlopen.xs, dlext=so, d_dlsymun=undef, ccdlflags='-rdynamic'
    cccdlflags='-fpic', lddlflags='-shared -L/usr/local/lib'


Characteristics of this binary (from libperl):
  Built under linux
  Compiled at Jul 22 1999 21:20:02
  @INC:
    /usr/lib/perl5/5.00503/i586-linux
    /usr/lib/perl5/5.00503
    /usr/lib/perl5/site_perl/5.005/i586-linux
    /usr/lib/perl5/site_perl/5.005
    .

Found compiler g77
ExtUtils::F77: Using system=Generic compiler=G77
Checking for gcc in disguise
Compiler is gcc version egcs-2.91.66 19990314/Linux (egcs-1.1.2
release)ExtUtils::F77: Validating -L/usr/lib
 -L/usr/lib -lf2c -lm -L/usr/lib/gcc-lib/i486-linux/egcs-2.91.66 -lgcc   [ok]
ExtUtils::F77: Compiler: g77
ExtUtils::F77: Cflags: -O
Writing Makefile for PGPLOT
Warning: prerequisite ExtUtils::F77 1.11 not found at (eval 1) line 220.


cc -c -I/usr/local/pgplot -I/home/aaossm/kgb/soft/pgplot/bld -I/usr/local/pgplot
-Dbool=char -DHAS_BOOL -I/usr/local/include -O2 -pipe    -DVERSION=\"2.15\"
-DXS_VERSION=\"2.15\" -fpic -I/usr/lib/perl5/5.00503/i586-linux/CORE  PGPLOT.c
Running Mkbootstrap for PGPLOT ()
chmod 644 PGPLOT.bs
LD_RUN_PATH="/usr/local/pgplot:/usr/X11/lib:/usr/lib:/usr/lib/gcc-lib/i486-linux/egcs-2.91.66"
cc -o blib/arch/auto/PGPLOT/PGPLOT.so  -shared -L/usr/local/lib PGPLOT.o
-L/usr/local/pgplot -L/usr/local/pgplot -L/usr/local/lib -lcpgplot -lpgplot
-L/usr/X11/lib -L/usr/X11R6/lib -lX11 -L/usr/lib -L/usr/lib -lf2c -lm
-L/usr/lib/gcc-lib/i486-linux/egcs-2.91.66 -lgcc
chmod 755 blib/arch/auto/PGPLOT/PGPLOT.so
cp PGPLOT.bs blib/arch/auto/PGPLOT/PGPLOT.bs
chmod 644 blib/arch/auto/PGPLOT/PGPLOT.bs
Manifying blib/man3/PGPLOT.3pm

PERL_DL_NONLAZY=1 /usr/bin/perl -Iblib/arch -Iblib/lib
-I/usr/lib/perl5/5.00503/i586-linux -I/usr/lib/perl5/5.00503 test.pl
Default Device for plot tests [recommend /XSERVE] ?

 ============== Running test1.p ==============
Can't load 'blib/arch/auto/PGPLOT/PGPLOT.so' for module PGPLOT:
/usr/local/pgplot/libpgplot.so: undefined symbol: G77_getenv_0 at
/usr/lib/perl5/5.00503/i586-linux/DynaLoader.pm line 169, <STDIN> chunk 1.

 at test1.p line 3
 BEGIN failed--compilation aborted at test1.p line 3, <STDIN> chunk 1.

II. LINUX SUSE 6.0 INSTALLATION CONFIGURATION WITHOUT  PROBLEMS:

Summary of my perl5 (5.0 patchlevel 5 subversion 2) configuration:
  Platform:
    osname=linux, osvers=2.0.36, archname=i586-linux
    uname='linux einstein 2.0.36 #79 tue jan 19 12:41:20 met 1999 i686 unknown '

    hint=recommended, useposix=true, d_sigaction=define
    usethreads=undef useperlio=undef d_sfio=undef
  Compiler:
    cc='cc', optimize='-O2 -pipe', gccversion=egcs-2.91.60 19981201 (egcs-1.1.1
release)
    cppflags='-Dbool=char -DHAS_BOOL -I/usr/local/include'
    ccflags ='-Dbool=char -DHAS_BOOL -I/usr/local/include'
    stdchar='char', d_stdstdio=define, usevfork=false
    intsize=4, longsize=4, ptrsize=4, doublesize=8
    d_longlong=define, longlongsize=8, d_longdbl=define, longdblsize=12
    alignbytes=4, usemymalloc=n, prototype=define
  Linker and Libraries:
    ld='cc', ldflags =' -L/usr/local/lib'
    libpth=/usr/local/lib /lib /usr/lib
    libs=-lnsl -lndbm -lgdbm -ldb -ldl -lm -lc -lposix -lcrypt
    libc=, so=so, useshrplib=false, libperl=libperl.a
  Dynamic Linking:
    dlsrc=dl_dlopen.xs, dlext=so, d_dlsymun=undef, ccdlflags='-rdynamic'
    cccdlflags='-fpic', lddlflags='-shared -L/usr/local/lib'


Characteristics of this binary (from libperl):
  Built under linux
  Compiled at Jan 27 1999 12:19:30
  @INC:
    /usr/lib/perl5/5.00502/i586-linux
    /usr/lib/perl5/5.00502
    /usr/lib/perl5/site_perl/5.005/i586-linux
    /usr/lib/perl5/site_perl/5.005
    .
Found compiler g77
ExtUtils::F77: Using system=Linux compiler=G77
Checking for gcc in disguise
Compiler is gcc version egcs-2.91.60 19981201 (egcs-1.1.1 release)ExtUtils::F77:
Validating -L/usr/lib
 -L/usr/lib -lf2c -lm -L/usr/lib/gcc-lib/i486-linux/egcs-2.91.60 -lgcc   [ok]
ExtUtils::F77: Compiler: g77
ExtUtils::F77: Cflags: -O
Writing Makefile for PGPLOT

cc -c -I/home/aaossm/kgb/soft/pgplot/bld -I/usr/local/pgplot -Dbool=char
-DHAS_BOOL -I/usr/local/include -O2 -pipe    -DVERSION=\"2.11\"
-DXS_VERSION=\"2.11\" -fpic -I/usr/lib/perl5/5.00502/i586-linux/CORE  PGPLOT.c
Running Mkbootstrap for PGPLOT ()
chmod 644 PGPLOT.bs
LD_RUN_PATH="/usr/local/pgplot:/usr/X11/lib:/usr/lib:/usr/lib/gcc-lib/i486-linux/egcs-2.91.60"
cc -o blib/arch/auto/PGPLOT/PGPLOT.so  -shared -L/usr/local/lib PGPLOT.o
-L/usr/local/pgplot -L/usr/local/pgplot -L/usr/local/lib -lcpgplot -lpgplot
-L/usr/openwin/lib -L/usr/X11/lib -L/usr/X11R6/lib -lX11 -L/usr/lib -L/usr/lib
-lf2c -lm -L/usr/lib/gcc-lib/i486-linux/egcs-2.91.60 -lgcc
chmod 755 blib/arch/auto/PGPLOT/PGPLOT.so
cp PGPLOT.bs blib/arch/auto/PGPLOT/PGPLOT.bs
chmod 644 blib/arch/auto/PGPLOT/PGPLOT.bs
Manifying blib/man3/ExtUtils::F77.3pm
Manifying blib/man3/PGPLOT.3pm


description of installation of suse 6.0, where
pgperl is running successfully, the packages
installed resemble those in suse 6.2 where
pgperl does not run ...


[i] aalibdev  Development package for aalib                  0xxMount point
x
x [i] autoconf  An m4 macro package                            0xx
Freex
x [i] automake  Tool for automatically generating GNU style Makhxx/
x
x [i] bin86     8086 assembler and linker                      hxx
468.2 Mx
x [i] binutils  GNU binutils                                   hxx/dosc
x
x [i] bison     GNU bison parser generator                     hxx
36.0 Mx
x [i] bwbasic   There is Basic under Linux, too                hxx/dosd
x
x [ ] clisp     A Common-Lisp interpreter                      hxx
188.8 Mx
x [ ] cvs       Concurrent Versions System                     hxx/dose
x
x [ ] efence    ElectricFence                                  hxx
13.8 Mx
x [i] egcs      the egcs-compiler                              hxx/dosf
x
x [i] f2c       A Fortran-77 to C translator                   hxx
76.1 Mx
x [i] f2caout   a.out version of libf2c                        hxx/dosg
x
x [i] flex      flex - fast lexical analyzer generator   [i] flex      flex
- fast lexical analyzer generator         hxxMount point  x
x [ ] fpk       Free Pascal Compiler                           hxx
Freex
x [i] g77       GNU Fortran Compiler                           0xx/
x
x [i] gcc       The GNU C compiler and support files           0xx
468.2 Mx
x [ ] gccfront  frontend for gcc-2.7.2.x                       hxx/dosc
x
x [i] gcl       GNU Common Lisp                                hxx
36.0 Mx
x [i] gdb       The GNU debugger                               hxx/dosd
x
x [i] gdlib     Gif-Manipulating Library                       hxx
188.8 Mx
x [i] gettext   Tools for National Language Support (NLS)      hxx/dose
x
x [i] gforth    GNU Forth                                      hxx
13.8 Mx
x [i] global    common source code tag system                  hxx/dosf
x
x [i] gmp       GNU MP library                                 hxx
76.1 Mx
x [i] gnats     GNATS - Problem Report Management System       hxx/dosg
x
x [i] gobjc     GNU objective C Compiler                      [i] gobjc
GNU objective C Compiler                       hxxMount point  x
x [ ] gpc       GNU Pascal Compiler                            hxx
Freex
x [i] gpp       GNU C++ Compiler                               hxx/
x
x [i] guavac    A free compiler for the Java language          hxx
468.2 Mx
x [i] guile     GNU's Ubiquitous Intelligent Language for Exten0xx/dosc
x
x [ ] icmake    A Maker for C-Fans                             0xx
36.0 Mx
x [ ] indent    formats C source code                          hxx/dosd
x
x [ ] java      Java Developers Kit                            hxx
188.8 Mx
x [ ] javarunt  Java Runtime Environment                       hxx/dose
x
x [ ] joystick  joystick support (kernel module and binaries)  hxx
13.8 Mx
x [ ] jresep    Java Runtime Environment                       hxx/dosf
x
x [ ] kaffe     A virtual machine to run Java(tm) code         hxx
76.1 Mx
x [i] lclint    LCLint - a tool for statically checking C progrhxx/dosg
x
x [i] leda      a library of efficient data types and algorithmh [i] leda
a library of efficient data types and algorithmhxxMount point  x
x [i] libc      Libraries for the C compiler                   hxx
Freex
x [i] libd      Profiling and Debugging versions of libc.      hxx/
x
x [i] libgpp    C++-library                                    hxx
468.2 Mx
x [i] libgpp27  old version of the c++ libraries               hxx/dosc
x
x [i] libobjc   libobjects                                     hxx
36.0 Mx
x [i] libtool   Tool to build "shared libraries"               0xx/dosd
x
x [i] libxml    Library to manipulate XML files                0xx
188.8 Mx
x [i] libxmld   libxml development package                     hxx/dose
x
x [i] linclude  Include files for the kernel                   hxx
13.8 Mx
x [ ] linux     Rest of the kernel source code.                hxx/dosf
x
x [ ] lx_glibc  kernel-includes for glibc build                hxx
76.1 Mx
x [ ] lx_hack   Source of the newest hacker's kernel           hxx/dosg
x
x [ ] lx_large  Kernel sources for big servers.                 [ ] lx_large
Kernel sources for big servers.                hxxMount point  x
x [ ] lx_suse   The sources of the SuSE kernel                 hxx
Freex
x [i] make      GNU make command                               hxx/
x
x [ ] mico      Mico is CORBA                                  hxx
468.2 Mx
x [ ] minigcc   The GCC Preprocessor without the C-Compiler    hxx/dosc
x
x [ ] mocka     Modula-2 compiler                              hxx
36.0 Mx
x [ ] mtc       Modula-2 / C Converter                         hxx/dosd
x
x [i] nasm      Netwide Assembler (an x86 assembler)           hxx
188.8 Mx
x [ ] orbit     A high-performance CORBA ORB                   0xx/dose
x
x [ ] orbitdev  The ORBit development environment              0xx
13.8 Mx
x [ ] p2c       A Pascal to C translator.                      hxx/dosf
x
x [i] patch     GNU patch program                              hxx
76.1 Mx
x [ ] pccts     Purdue Compiler Construction Tool Set          hxx/dosg
x
x [i] pmake     BSD make                                       x [i] pmake
BSD make                                       hxxMount point  x
x [i] prcs      PRCS -- Project Revision Control System        hxx
Freex
x [i] python    Python Interpreter                             hxx/
x
x [i] rcs       Revision Control System                        hxx
468.2 Mx
x [ ] scheme    UMB Scheme                                     hxx/dosc
x
x [i] slang     Display control                                hxx
36.0 Mx
x [ ] smaltalk  GNU Smalltalk                                  hxx/dosd
x
x [ ] smeiffel  SmallEiffel                                    hxx
188.8 Mx
x [i] strace    Trace system calls of a program.               hxx/dose
x
x [ ] svgaaout  Svgalib Super-VGA Graphics Library (a.out)     hxx
13.8 Mx
x [i] svgalib   Svgalib Super-VGA Graphics Library             0xx/dosf
x
x [ ] swi_pl    SWI-Prolog distribution                        0xx
76.1 Mx
x [i] toolpack  extensive collection of tools for Fortran progrhxx/dosg
x
x [ ] tvision   tvision                                         [i] slang
Display control                                hxxMount point  x
x [ ] smaltalk  GNU Smalltalk                                  hxx
Freex
x [ ] smeiffel  SmallEiffel                                    hxx/
x
x [i] strace    Trace system calls of a program.               hxx
468.2 Mx
x [ ] svgaaout  Svgalib Super-VGA Graphics Library (a.out)     hxx/dosc
x
x [i] svgalib   Svgalib Super-VGA Graphics Library             hxx
36.0 Mx
x [ ] swi_pl    SWI-Prolog distribution                        hxx/dosd
x
x [i] toolpack  extensive collection of tools for Fortran progrhxx
188.8 Mx
x [ ] tvision   tvision                                        hxx/dose
x
x [ ] tya       TYA is a 100% inofficial JIT-compiler          hxx
13.8 Mx
x [ ] xclass    Linux Explorer + library                       hxx/dosf
x
x [ ] xscheme   An object-oriented scheme                      hxx
76.1 Mx
x [i] yacc      BSD yacc                                       0xx/dosg
x
x [ ] yodl      Yet Oneother Document Language                 0x [ ] ddd
Debugger with graphical user interface         0xxMount point  x
x [ ] dlgedit   QT Dialog Editor                               0xx
Freex
x [ ] ezwgl     ezwgl                                          0xx/
x
x [ ] iv        InterViews - a GUI.                            0xx
468.2 Mx
x [ ] qtcompat  Compatibility includes for older QT programs   0xx/dosc
x
x [ ] qtdevel   QT development environment                     0xx
36.0 Mx
x [ ] qtext     QT extensions                                  0xx/dosd
x
x [i] qtlib     QT runtime libraries                           0xx
188.8 Mx
x [ ] vtk       Visualization ToolKit                          hxx/dose
x
x [ ] vtkdata   Visualization ToolKit - Datafiles              hxx
13.8 Mx
x [ ] wxwdemo   Demo programs for wxwin                        hxx/dosf
x
x [ ] wxwdocht  Documentation for wxwin in HTML                hxx
76.1 Mx
x [ ] wxwdocps  Documentation of wxwin in PostScript           hxx/dosg
x
x [ ] wxwin     GUI Library for Motif, Openlook and MS-Windows  [ ] wxwin
GUI Library for Motif, Openlook and MS-Windows hxx       36.0 Mx
x [ ] wxwstat   Static libraries for package wxwin             0xx/dosd
x
x [ ] wxxt      Port of wxwin with motif look-and-feel         0xx
188.8 Mx
x [i] xforms    Forms Library                                  0xx/dose
x
x [ ] xtpanel   Interface Builder using scripts                0xx
13.8 Mx
x [i] xwb       software development environment for openwin   0xx/dosf
x
x [i] xwpe      A X-window programming environment             0xx
76.1 Mx
x [i] xxgdb     xxgdb, user interface to the GNU debugger under0xx/dosg
x
x [ ] ygl       a GL graphics library with sample file         0


linux base system (nearly) everything
no source packages

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From kristian.nielsen at risoe.dk  Tue Jan 18 22:32:40 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 18 Jan 2000 22:32:40 +0100
Subject: help
In-Reply-To: <000801bf60cc$e744bda0$940a26ca@ciae.ac.cn> (message from guolp
	on Mon, 17 Jan 2000 17:26:09 +0800)
Message-ID: <mailman.86.1511353198.451.mcstas-users@mailman2.mcstas.org>

> I've just read your paper " McStas, a general software package for
> neutron ray-tracing simulations" published on Neutron News
> 10(1999),20-23. I'm very interested in Monte Carlo simulations of
> neutron scattering spectrometer. We are designing several
> spectrometers on China Advanced Research Reactor(CARR) under
> construction. These spectrometers include a high resolution powder
> diffractometer, a neutron reflectometer, a high Q diffractometer, a
> cold and a thermal neutron guide,and a three axis spectrometer.I hope
> I could use ray-tracing simulations technique and your software McStas
> in our design. My colleagues and I may need your help. First, what is
> ray-tracing simulations? Could you tell me some references which
> introduces this technique in details? Secondly, can this technique be

Well, maybe the best place to start would be to look at the McStas
manual. This may be downloaded from the McStas web page

    http://neutron.risoe.dk/mcstas/

If you have problems obtaining it, I can send you a paper copy.

> used in design of all of our spectrometers mentioned above?

Yes, McStas should be able to handle all of the instruments you
mentioned.

> Thirdly,besides in design, does this technique has any other usages in
> the running of our spectrometer after built up it in the future?  I

Yes. It can be used to select between different configuration before
starting an experiment, for example to get the best possible
signal/background ratio. And it can be used to compute eg. the
resolution function of an instrument which can be used to analyse
experiment data.

> hope you could give some help to me. I'm looking forward to hearing
> from you.

Do you know Sun Kai and Dong Feng Chen? If you do, you may be interested
to know that they have also started to look at Monte Carlo and McStas.

I hope this helps.

 - Kristian.





From farhi at ill.fr  Tue Jan 25 12:31:55 2000
From: farhi at ill.fr (Farhi)
Date: Tue, 25 Jan 2000 12:31:55 +0100
Subject: Cristallographica
Message-ID: <388D89AB.D4EB590@ill.fr>

By the way,

the program Cristallographica only works on PC's. Do you know other ways
to generate the crystal diffraction patterns ? what file format is it
exactly (CIF ?)

Thanks. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue des Martyrs, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From kristian.nielsen at risoe.dk  Tue Jan 25 12:37:46 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 25 Jan 2000 12:37:46 +0100
Subject: Cristallographica
In-Reply-To: <388D89AB.D4EB590@ill.fr> (message from Farhi on Tue, 25 Jan 2000
	12:31:55 +0100)
Message-ID: <mailman.87.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Tue, 25 Jan 2000 12:31:55 +0100
> From: Farhi <farhi at ill.fr>

> the program Cristallographica only works on PC's. Do you know other ways
> to generate the crystal diffraction patterns ? what file format is it
> exactly (CIF ?)

Hm, I am sorry to hear that Crystallographica is Windows only ...
Anyway, the file is just straight ASCII, list of (h,k,l) and the
structure factor |F|**2. Like this

h  k  l  dummy  dummy dummy F2
h  k  l  dummy  dummy dummy F2
h  k  l  dummy  dummy dummy F2
...

Crystallographica output the "dummy"'s, but they are not used. It should
be quite easy to write a program that inputs the atoms in the unit cells
and does the sums in the textbook expression for F2.

Anyway, this information will be in the manual (of course).

 - Kristian.






From stuart at studsvik.uu.se  Fri Feb  4 16:58:40 2000
From: stuart at studsvik.uu.se (stuart)
Date: Fri, 04 Feb 2000 16:58:40 +0100
Subject: Calulating intensities
Message-ID: <389AF72F.384B4B99@studsvik.uu.se>

Hi

I was trying to compare the intensities given from a simulation when
using different energy/wavelength neutrons, and have been trying to
understand the way in which the monochromator mosaicity would affect the
number reflected, for those different incident energies/wavelengths.

Should the energy spread of the neutrons, from the source be different
for each energy simulated in order to give an identical wavelength
spread, incident upon the monochromator?  Or maybe I'm thinking about it
the wrong way!

Stuart Rycroft,
NFL Studsvik



From kristian.nielsen at risoe.dk  Mon Feb  7 09:21:32 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: Mon, 07 Feb 2000 09:21:32 +0100
Subject: New release v1.2 of McStas
Message-ID: <01JLMDA0XPWA90WXIE@risoe.dk>

I am pleased to announce that McStas v1.2 has been released and may be
downloaded from the web site:

    http://neutron.risoe.dk/mcstas/

The main new features include a new graphical user interface called
mcgui as well as an extended component library including a general
single crystal sample, adaptive importance sampling neutron source,
resolution calculation sample, etc. See the CHANGES file in the
distribution for details on what is new in v1.2.

All McStas users are encouraged to upgrade to the new version. Users
that have installed one of the alpha/beta versions of McStas prior to
McStas version 1.2 are especially encouraged to upgrade as these
pre-releases contain known bugs that are fixed in version 1.2.

As usual, please report any problems so that they may be fixed in a
later version.

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790



From kristian.nielsen at risoe.dk  Mon Feb  7 11:34:39 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: Mon, 07 Feb 2000 11:34:39 +0100
Subject: Calulating intensities
In-Reply-To: <389AF72F.384B4B99@studsvik.uu.se>
 (message from stuart on Fri, 04 Feb 2000 16:58:40 +0100)
Message-ID: <01JLMHX3CV9U919Z2M@risoe.dk>

> Date: Fri, 04 Feb 2000 16:58:40 +0100
> From: stuart <stuart at studsvik.uu.se>

> I was trying to compare the intensities given from a simulation when
> using different energy/wavelength neutrons, and have been trying to
> understand the way in which the monochromator mosaicity would affect the
> number reflected, for those different incident energies/wavelengths.
> 
> Should the energy spread of the neutrons, from the source be different
> for each energy simulated in order to give an identical wavelength
> spread, incident upon the monochromator?  Or maybe I'm thinking about it
> the wrong way!

I am not quite sure here about what you have in mind, but it sounds like
your problem is that the neutron source you use specifies the spectrum
in terms of energy, while what you need is to specify it in terms of
wavelength. In that case you should try to use the Source_flux_lambda
component that is included in the just-released McStas version 1.2 (I
assume you use McStas though you did not mention it explicitly). That
will give you easily the same wavelength spread at all wavelengths.

More generally, the prediction of absolute reflectivity at different
wavelengths of mosaic crystals is (as far as I know) a very hard
problem. Complications arise because both primary and secondary
extinction becomes important, and these depend strongly on the precise
characteristics on the mosaic (a simple Gaussian model may not be
sufficient). Samuel Werner discusses the problem in his 1965 PhD thesis
(I think the title is "The multiple Bragg scattering of neutrons from
mosaic crystals").

Hope this helps,

 - Kristian.



From jankner at anl.gov  Tue Feb  8 18:42:24 2000
From: jankner at anl.gov (Ankner, John)
Date: Tue, 08 Feb 2000 11:42:24 -0600
Subject: 3d detectors
Message-ID: <A0E27DD848C1D211AE10006097C9C0BB058847@exchmail.pns.anl.gov>

Kristian,
     I modified your PSD_monitor routine to handle time-of-flight data
(called PSDTOF_monitor.comp).  The new detector generates data in x, y, and
t and I find I now have a major file-size problem.  For example, a 140?140
PSD_monitor generates about a 150 kB file.  If we divide 16.7 msec (1/60 for
the SNS source) into 10 mu-sec bins, we need 1670?150 kB or several hundred
MB.  These files are quite sparse, so there should be great gains to be made
via data compression.  In addition, the ideal way to view this data would be
by looking at x-y plots over a specified range of time channels.  This
viewing would best be done interactively.  In other words, import the entire
data set into a viewer to which one can specify a range of time channels.
My impression is that Nexus can help with both the compression and the
viewing.  Do you have any plans for generating Nexus files?  I will look
into this, but I suspect you are the most-qualified person for the job.
John
P.S. Is the source code for the DETECTOR_OUT_2D macro available?


From kristian.nielsen at risoe.dk  Wed Feb  9 09:51:34 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: Wed, 09 Feb 2000 09:51:34 +0100
Subject: 3d detectors
In-Reply-To: <A0E27DD848C1D211AE10006097C9C0BB058847@exchmail.pns.anl.gov>
 (jankner@anl.gov)
Message-ID: <01JLP6WYEEEQ91B0AW@risoe.dk>

> Kristian,
>      I modified your PSD_monitor routine to handle time-of-flight data
> (called PSDTOF_monitor.comp).  The new detector generates data in x, y, and
> t and I find I now have a major file-size problem.  For example, a 140?140
> PSD_monitor generates about a 150 kB file.  If we divide 16.7 msec (1/60 for
> the SNS source) into 10 mu-sec bins, we need 1670?150 kB or several hundred
> MB.  These files are quite sparse, so there should be great gains to be made

OK, that would be a problem.

The current method needs to store one double precision floating point
number for each bin (8 bytes) in memory during the simulation. This
would be 260 Mb of RAM needed in your case which is a lot, but not
totally unreasonable. To compute error estimates the current method
needs three times that amount which is quite a lot. However, going to
single precision is quite dangerous for large number of neutron
histories (~10e9). Once the computation finishes, converting to single
precision is fine, of course.

I already had plans to implement an optional binary output format. This
would output your detector data as a single precision binary file (130Mb
in your case). This would then subsequently be converted to NeXuS. This
is something I could implement for you quickly (a few weeks) if needed.

> via data compression.  In addition, the ideal way to view this data would be
> by looking at x-y plots over a specified range of time channels.  This
> viewing would best be done interactively.  In other words, import the entire
> data set into a viewer to which one can specify a range of time channels.
> My impression is that Nexus can help with both the compression and the
> viewing.  Do you have any plans for generating Nexus files?  I will look
> into this, but I suspect you are the most-qualified person for the job.

Your example clearly shows the use of writing NeXuS directly from the
simulation, using its build-in data compression algorithms. This would
appear to be quite useful here. I will think some more about it, but
that will take somewhat longer to implement.

Are you saying that a suitable general viewer is already available for
the NeXuS/HDF format? That would be great, obviously it will never be
possible to create all the visualization tools we need specifically for
McStas. If good NeXuS/HDF tools are available, I will want to accelerate
the implementation of NeXuS in McStas.

> P.S. Is the source code for the DETECTOR_OUT_2D macro available?

Yes, it is found in the files mcstas-r.h and mcstas-r.c (located in the
lib/ subdirectory of the distribution). Obviously we need to include a
DETECTOR_OUT_3D macro as well. Send me your code when you finish it or
get stuck, and I will look at it.

Good luck, it sounds like you are doing great work!

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790



From kristian.nielsen at risoe.dk  Wed Feb  2 10:25:20 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 2 Feb 2000 10:25:20 +0100
Subject: Windows compilation
In-Reply-To: <A0E27DD848C1D211AE10006097C9C0BB058831@exchmail.pns.anl.gov>
	(jankner@anl.gov)
Message-ID: <mailman.88.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Tue, 01 Feb 2000 09:06:01 -0600
> From: "Ankner, John" <jankner at anl.gov>

> Kristian,

> goes well, except that neither I nor the Visual C++ 5.0 compiler/linker can
> locate a main() function.  In my limited knowledge of C, I believe we need

The main() function is located in the file "instrument.tab.c". Probably
you missed this file because of file name mangling when copying between
Linux and Windows. You also need the file "lex.yy.c". Maybe you should
rename them to something without two dots.

> In addition, what function does the mcstas-r.c code perform?  Attempting to
> compile it with the rest causes many error messages.  I have therefore
> omitted it.

That is right, it should not be included. It is used in the simulations
generated by mcstas, not in mcstas itself.

I hope this helps,

 - Kristian.





From jankner at anl.gov  Tue Feb  1 16:06:01 2000
From: jankner at anl.gov (Ankner, John)
Date: Tue, 01 Feb 2000 09:06:01 -0600
Subject: Windows compilation
Message-ID: <A0E27DD848C1D211AE10006097C9C0BB058831@exchmail.pns.anl.gov>

Kristian,
     Having now encountered sufficient difficulties in trying to compile a
new PSD TOF detector on the Linux box, I am now attempting to install mcstas
on my NT box.  I followed the directions in your previous message and all
goes well, except that neither I nor the Visual C++ 5.0 compiler/linker can
locate a main() function.  In my limited knowledge of C, I believe we need
this.  Let me know if there is something subtle going on (trivial being more
likely).  FYI, here is the linker error message:


--------------------Configuration: mcstas - Win32 Debug--------------------
Linking...
LIBCD.lib(crt0.obj) : error LNK2001: unresolved external symbol _main
Debug/mcstas.exe : fatal error LNK1120: 1 unresolved externals
Error executing link.exe.

mcstas.exe - 2 error(s), 0 warning(s)


In addition, what function does the mcstas-r.c code perform?  Attempting to
compile it with the rest causes many error messages.  I have therefore
omitted it.
Thanks,
John




From kristian.nielsen at risoe.dk  Thu Feb  3 11:40:08 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 3 Feb 2000 11:40:08 +0100
Subject: mcgui on non linux machines
In-Reply-To: <389950D1.6E1F6A81@ill.fr> (message from Farhi on Thu, 03 Feb
	2000 10:56:33 +0100)
Message-ID: <mailman.89.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Thu, 03 Feb 2000 10:56:33 +0100
> From: Farhi <farhi at ill.fr>

> No problems to get back ? Perhaps could you see the top of the
> Mont-Blanc flying over the clouds ?

No problems, but there were too many clouds to see anything (or maybe I
was in the wrong side of the plane).

> I've improved my Flux_adapter and Optimizer. I think it is possible to
> use more that one Monitor Optimizer, in order to optimize simulation
> according to various criteria. Each neutron that reach a
> Monitor_Optimizer increases the Source efficiency, even if it is counted
> more that once during tracing. If the neutron reaches two
> Monitor_Optimizer, it will count twice in the optimization, and this is
> fair.

Sounds good!

> I've experimented a major pb for mcgui. When on a Linux machine, no pbs
> because these machines use the same compilers and options for linker...
> But when running for instance on SGI/IRIX, it leads to a core because
> one has to use the IRIX cc compiler, with specific options. gcc crashes.
> And for HP or DEC machines, htere are even more restricted options (to
> force ANSI code for instance).

Ok, there is (or should be) a way to handle this. The command used by
mcgui to compile is the same command used to compile mcstas during
installation. If this is wrong, McStas must be re-installed with the
proper compile commands.

The way to do this is

  rm config.cache        # To remove any old, wrong settings
  setenv CC cc           # Name of compiler to use
  setenv CFLAGS "-O -g"  # Necessary compiler options
  ./configure
  make install

By setting CC and CFLAGS before configure, mcgui should pick up the
right commands. Of course, there should be a way to override this after
installation, I will work on that.

By the way, I thought I had fixed the problem on the DEC machines, if
not please send details.

> I've copied the latest versions of mcstas package on the Web page, as
> well as the new components definitions. It seems however that not all
> components have a valid header yet. The components that I had installed
> before did ! I think I get them back on the web now, so that you can get
> them, and compare/add headers and MCDISPLAY sections. If you do not have
> time for that, I think I can do the 'homogeneisation' today or tomorrow.
> Then I'll send you the new clean components.

Indeed, I seem to have forgotten MCDISPLAY in five components: Chopper,
First_Chopper, Monitor_4PI, Source_div, and V_selector.comp. Thanks for
the notice.

However, I could not find any official components without headers (only
did a quick check). I think perhaps you are thinking of some of the
components that were in the BETA releases I send you, but that were
removed from the final release. Perhaps they just got left in your
/usr/local/lib/mcstas directory? Otherwise let me know the names, and I
will fix it.

Anyway, thanks for the comments. It was good to see you at the ILL!

 - Kristian.





From farhi at ill.fr  Thu Feb  3 10:56:33 2000
From: farhi at ill.fr (Farhi)
Date: Thu, 03 Feb 2000 10:56:33 +0100
Subject: mcgui on non linux machines
Message-ID: <389950D1.6E1F6A81@ill.fr>

Hello Kristian,

No problems to get back ? Perhaps could you see the top of the
Mont-Blanc flying over the clouds ?
I've improved my Flux_adapter and Optimizer. I think it is possible to
use more that one Monitor Optimizer, in order to optimize simulation
according to various criteria. Each neutron that reach a
Monitor_Optimizer increases the Source efficiency, even if it is counted
more that once during tracing. If the neutron reaches two
Monitor_Optimizer, it will count twice in the optimization, and this is
fair.

I've experimented a major pb for mcgui. When on a Linux machine, no pbs
because these machines use the same compilers and options for linker...
But when running for instance on SGI/IRIX, it leads to a core because
one has to use the IRIX cc compiler, with specific options. gcc crashes.
And for HP or DEC machines, htere are even more restricted options (to
force ANSI code for instance).

I've copied the latest versions of mcstas package on the Web page, as
well as the new components definitions. It seems however that not all
components have a valid header yet. The components that I had installed
before did ! I think I get them back on the web now, so that you can get
them, and compare/add headers and MCDISPLAY sections. If you do not have
time for that, I think I can do the 'homogeneisation' today or tomorrow.
Then I'll send you the new clean components.

Cheers. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue des Martyrs, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From kristian.nielsen at risoe.dk  Thu Feb  3 12:39:09 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 3 Feb 2000 12:39:09 +0100
Subject: SINS slides?
Message-ID: <mailman.90.1511353198.451.mcstas-users@mailman2.mcstas.org>

Hi Thomas,

It was good to see you at the ILL. I was very impressed with the work
you have done so far, it is very ambitious I think compared to what I
have seen in terms of simulations elsewhere. It also clearly
demonstrates the need for a simulation program like McStas to be very
extendible.

We are several people here at Risoe interested in having a copy of the
slides you presented at the workshop at ILL. Would it be possible for
you to send a copy (either electronically or on paper)?

Also thanks for the very nice tour of the new D20 you gave me.

 - Kristian.





From hansen at ill.fr  Thu Feb  3 13:01:12 2000
From: hansen at ill.fr (Thomas C Hansen)
Date: Thu, 03 Feb 2000 13:01:12 +0100
Subject: Adapt_check
Message-ID: <38996E05.B5D63307@ill.fr>

I'm not sure, but I think it's Adapt_check which makes my new simulation stop
without error messages after about 100 neutrons passed (sometimes with finite
weight p - due to the flux greater than 1 - also in Adapt_check). Debugging
won't be easy, but if you could file me some general hints for the use of
Source_adapt/Adapt_check, that may already be helpful enough.

Thanks a lot in advance,

Thomas






From hansen at ill.fr  Thu Feb  3 19:02:14 2000
From: hansen at ill.fr (Thomas C Hansen)
Date: Thu, 03 Feb 2000 19:02:14 +0100
Subject: Adapt_check
References: <01JLH14N02CK9189QK@risoe.dk>
Message-ID: <3899C299.5E1C5DE3@ill.fr>

I got it: As with the new Source_adapt, weights greater one are possible, and as
I had - stupid enough - in one of my components for debugging reasons "if (p>1)
exit(1);", the program stops quite early. That does not mean that I am error
free now, but ... we will see ...

Have a nice evening,

Thomas

Kristian Nielsen wrote:

> Hi Thomas,
>
> Thanks for the copy of your slides, which arrived and printed without
> problems.
>
> As to the Source_adapt/Adapt_check combination, probably the easiest
> would be if you could send me the files you used (and a set of input
> parameters that show the problems). Then I could probably quickly find
> the cause of your problem.
>
> The Source_adapt/Adapt_check components will be documented in the McStas
> v1.2 manual, which I will release in a few days.
>
>  - Kristian.

--
Dr. Thomas C HANSEN, Instrument Scientist D20, Diffraction Group
Institut Max von Laue-Paul Langevin, BP 156, 38042 Grenoble C?dex 9, France
ILL4-1st floor room 100, Phone +33(0)476207044, Fax +33(0)476207648
mailto:hansen at ill.fr, http://www.ill.fr/YellowBook/D20
Private: 13, all?e des ?tangs, 38240 Meylan, France, +33(0)476180553







From kristian.nielsen at risoe.dk  Tue Feb  8 11:02:41 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 8 Feb 2000 11:02:41 +0100
Subject: McStas PANDA simulation
In-Reply-To: <38959F90.10C0269C@physik.tu-dresden.de> (message from martin
	rotter on Mon, 31 Jan 2000 15:43:28 +0100)
Message-ID: <mailman.91.1511353198.451.mcstas-users@mailman2.mcstas.org>

Dear Martin,

Many thanks for the report you send me. I have made it available from
the McStas home page, at

    http://neutron.risoe.dk/mcstas/reflist.html

(see the bottom of the page). I am sure that it will be of use to other
users. I will also take a closer look, probably there will be some
suggestions for improving future versions of McStas. For one, I have
made a note to include a batch option (non-interactive postscript
output) in mcdisplay and mcplot.

It is clear that you have spent a great deal of effort on this work with
McStas!

Thanks,

 - Kristian.





From kristian.nielsen at risoe.dk  Thu Feb 10 09:03:39 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 10 Feb 2000 09:03:39 +0100
Subject: McStas installation and Perl
Message-ID: <mailman.92.1511353198.451.mcstas-users@mailman2.mcstas.org>

Dear Ron,

It was good to see you again at the ILL last week. Thanks for all your
work in organizing the workshop.

Last Tuesday, we discussed your problems with the location of the Perl
interpreter during the McStas install. We agreed that I should implement
a way for the user to explicitly set the path to Perl during the
installation.

Well, it turns out that this is already possible, I just did not realize
it! Before running the ./configure thing, the PERL environment variable
may be set to the complete path of the Perl executable to use:

    setenv PERL /my/special/perl
    ./configure --prefix=/my/prefix

The setting of PERL overrides configure's guess. It may be necessary to
remove configure's cache file,

    rm config.cache

I will document this in the INSTALL document and in the FAQ. Let me know
if you have any other trouble with this.

I will also be looking into the compiler warnings we discussed.

 - Kristian.





From Ralph_Gilles at Physik.TU-Muenchen.DE  Fri Feb 11 17:45:44 2000
From: Ralph_Gilles at Physik.TU-Muenchen.DE (Ralph Gilles)
Date: Fri, 11 Feb 2000 17:45:44 +0100
Subject: publications
Message-ID: <38A43CB8.5147F1CA@ph.tum.de>

Dear Kristian,

In past I was not so active in sending emails concerning your excellent
program (Georg Artus was combining our questions and comments).In the
mentioned papers below I mentioned you and your colleague Kim for your
excellent work and tried to motivate other people to use the program.
Today I received questions concerning the program from 'new cancidates
for McStas in future 'and this is the actual reason to write the email
and to thank again for the support and help in past.

Good luck ! I hope that I also helped you to spread the program over the
world.

greetings, Ralph

paper:

R. Gilles, G. Artus, J. Saroun, H. Boysen, H. Fuess
The new structure powder diffractometer at the FRM II in Garching
Commission on Powder Diffraction (1999), Newsletter No.22,12.

R. Gilles, G. Artus, J. Saroun, H. Boysen, H. Fuess
The new structure powder diffractometer at the FRM II in Garching
Physica B (2000), in print.

R. Gilles, J. Saroun, H. Boysen, H. Fuess
Monte Carlo Simulation for a neutron guide system of the new Structure
Powder Diffractometer at the FRM-II in Garching
Proceedings of the HERCULES X EuroConference 2000, Grenoble, submitted.

another 'one'  I am preparing

poster:

R. Gilles, H. Boysen, H. Fuess
Das Neue Strukturpulverdiffraktometer am FRM II
Deutsche Neutronenstreutagung 1999
May 25th ? 27th, Potsdam, Germany



--
Address:
Dr. Ralph Gilles
TU M?nchen
Reaktorstation
D-85747 Garching
phone.: 049-(0)89-289-14665
fax.: 049-(0)89-289-14666
e-mail: rgilles at ph.tum.de







From kristian.nielsen at risoe.dk  Mon Feb 14 10:00:19 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 14 Feb 2000 10:00:19 +0100
Subject: publications
In-Reply-To: <38A43CB8.5147F1CA@ph.tum.de> (message from Ralph Gilles on Fri,
	11 Feb 2000 17:45:44 +0100)
Message-ID: <mailman.93.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Fri, 11 Feb 2000 17:45:44 +0100
> From: Ralph Gilles <Ralph_Gilles at Physik.TU-Muenchen.DE>

> Dear Kristian,
> 
> In past I was not so active in sending emails concerning your excellent
> program (Georg Artus was combining our questions and comments).In the
> mentioned papers below I mentioned you and your colleague Kim for your

Thank you for the kind words and for the references. I have put the
references on the web page. It is very encouraging to hear about people
using the program with success, that is after all the whole motivation
for doing the work.

I am also happy to hear that other users are joining the project.

 - Kristian.





From kristian.nielsen at risoe.dk  Tue Feb 15 12:00:26 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 15 Feb 2000 12:00:26 +0100
Subject: Bugs in McStas/McGUI
In-Reply-To: <38A296BD.5136980A@ill.fr> (message from Farhi on Thu, 10 Feb
	2000 11:45:17 +0100)
Message-ID: <mailman.94.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Thu, 10 Feb 2000 11:45:17 +0100
> From: Farhi <farhi at ill.fr>

Hi Emmanuel and Ron,

I have fixed some of the points we discussed at my visit a few weeks
ago:

 - Compiler warnings on SGI.
 - Components stored in subdirectories (samples, optics, monitors,
   sources, misc).
 - Automatic generation of documentation (HTML web pages) from component
   header comments.
 - String values for instrument parameters.

The use of strings for instrument parameters was somewhat more involved
than I thought initially because of the need to handle it also in the
front-ends (mcgui), but I think it is solved now.

I can send you a new version if you want. There is still one serious
bug; because of the new subdirectory structure for components, users
installing the new version may end up with both old and new components
in the mcstas directory. This is bound to cause confusion and I have not
yet decided the correct way to solve it.

About your problems on the SGI:

> 1- When on a SGI machine, I launch mcgui with the example tutorial
> in14_tut (from web)
> 
> mica~farhi 32% mcgui in14_tut.instr
> Ambiguous use of expand => resolved to "expand" => at
> /usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1038.
> Ambiguous use of expand => resolved to "expand" => at
> /usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1075.

Hm, this warning addresses the syntax in the source for Perl/Tk. What
version of Perl/Tk is installed? Anyway, this sounds completely harmless
(but annoying anyway). It will probably go away if the "-w" switch in
the first line of mcgui.pl is removed (please tell me if it does).

> Then if I try to compile instrument
> mcstas -t -o in14_tut.out.c in14_tut.instr
> 
> Then I crashes (mcgui disappears, core dumped). No 'cc' call is
> displayed in mcgui, but I think the problem occurs here.
> The manual processing works ok.

> 2- When using the POLARISATION macro, mcstas warns about comps that do
> not handle that, but also crashes (seg fault) at the end.
> The '.c' file is generated anyway.

Not good! Unfortunately, I could not reproduce these two crashes. That
makes it quite difficult to give suggestions.

Would it be possible to re-establish my "nielsen" account at the ILL?
Then I could just log in and try it myself, and hopefully the cause
would be apparent in 10 minutes?

 - Kristian.





From farhi at ill.fr  Thu Feb 10 11:45:17 2000
From: farhi at ill.fr (Farhi)
Date: Thu, 10 Feb 2000 11:45:17 +0100
Subject: Bugs in McStas/McGUI
Message-ID: <38A296BD.5136980A@ill.fr>

Hy again

just a note to tell you about strange behaviours of McStas 1.2

1- When on a SGI machine, I launch mcgui with the example tutorial
in14_tut (from web)

mica~farhi 32% mcgui in14_tut.instr
Ambiguous use of expand => resolved to "expand" => at
/usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1038.
Ambiguous use of expand => resolved to "expand" => at
/usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1075.

Then if I try to compile instrument
mcstas -t -o in14_tut.out.c in14_tut.instr

Then I crashes (mcgui disappears, core dumped). No 'cc' call is
displayed in mcgui, but I think the problem occurs here.
The manual processing works ok.

2- When using the POLARISATION macro, mcstas warns about comps that do
not handle that, but also crashes (seg fault) at the end.
The '.c' file is generated anyway.

Cheers again. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue des Martyrs, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From ron at ill.fr  Mon Feb 14 13:56:11 2000
From: ron at ill.fr (Ron Ghosh)
Date: Mon, 14 Feb 2000 13:56:11 +0100
Subject: McStas installation and Perl
References: <01JLQJKNH5EK91C1U8@risoe.dk>
Message-ID: <38A7FB6B.BE28D4A6@ill.fr>

It was a great pleasure to see you again, Kristian.

Inevitably configure specialists have thought of the most improbable
mix of configurations! Thanks for the hints. 

Emmanual has hit a problem with the shared mcgui - I think he has told
you.  He is away at present.  I'll take it up with him when he returns
in a day or so. If
you have any suggestions I'd be interested to hear from you.

Best wishes, and keep on with the good work, Ron

-- 
Ron Ghosh, Institut Laue Langevin, B.P. 156    tel: +33-476207178
38042 Grenoble cedex 9, FRANCE                 fax: +33-476483906




From kristian.nielsen at risoe.dk  Wed Feb 16 10:46:54 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 16 Feb 2000 10:46:54 +0100
Subject: Bugs in McStas/McGUI
In-Reply-To: <38A94485.EBBD3D5A@ill.fr> (message from Farhi on Tue, 15 Feb
	2000 13:20:21 +0100)
Message-ID: <mailman.95.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Tue, 15 Feb 2000 13:20:21 +0100
> From: Farhi <farhi at ill.fr>

> you can use my login on firewall.ill.fr :

Ok, thanks.

> For the polarisation error, I will make some other checks when I got time.

Do not worry, I found the problem easily after logging in on mica. It
was a stupid cut-and-paste error.

Unfortunately, I was not able to debug the problems with mcgui. The ILL
firewall seems to completely block all X windows access in both
directions now (I think previously ILL-local applications could be
displayed on remote X terminals). So it looks like we have to debug
manually.

As a start, try to reproduce the crash inside the perl debugger. Start
mcgui with the command

    perl -d /usr/ill/bin/mcgui in14_tut.instr

and type

    r

to start the program. Then send the complete output when it crashes.

 - Kristian.





From kim.lefmann at risoe.dk  Tue Feb 15 13:04:22 2000
From: kim.lefmann at risoe.dk (Kim Lefmann)
Date: Tue, 15 Feb 2000 13:04:22 +0100 (CET)
Subject: mirror reflection
In-Reply-To: <38A93A10.265DA84F@psi.ch>
Message-ID: <Pine.LNX.3.96.1000215125142.27874D-100000@fys-lin-1.risoe.dk>

Dear Peter,

The mirror component should not be difficult to use if you realize that it
should be rotated 90 degrees around the Y-axis to be used in a usual
geometry. Unrotated, the mirror just intersects the neutron flight
direction (z) at right angles. Perhaps we should write this in the 
manual(!)

The bottom nearest corner of the mirror is placed in Origo of the local
cordinate system, so you need to shift the mirror with respect to the beam
centre by "yheight/2", if you see what I mean.

I can see that this is not really a convenient component to use. If you
work with it for a little while and tell us how exactly you would like it
to work, we will rebuild it for you in a short while.

Did you, by the way, notice that McStas release 1.2. is out now? There are
especially some improved graphical front ends and an adaptive source,
which could be useful for you.
 
Yours, Kim

---------------------------

Kim Lefmann

Dept. Cond. Matt. Phys. & Chem.
Risoe National Laboratory

Phone: +45 46 77 47 26
Fax:   +45 46 77 47 90

On Tue, 15 Feb 2000, Peter [iso-8859-1] B?ni wrote:

> Dear Kim
> 
> In McStas there exists a component for reflection from a mirror. Somehow 
> I do not know how to correctly use it. The definition for the size of
> the
> mirror and the coordinate system are not in the same spirit as for the
> monochromator component. Is this correct? Do you have an example for a
> simulation that uses a mirror? Could you send me an example, if you have
> one?
> 
> Best regards    Peter
> 
> 





From farhi at ill.fr  Wed Feb 16 14:09:55 2000
From: farhi at ill.fr (Farhi)
Date: Wed, 16 Feb 2000 14:09:55 +0100
Subject: Bugs in McStas/McGUI
References: <01JLZ0W0AJMM91DJFO@risoe.dk>
Message-ID: <38AAA1A3.88FAE9AE@ill.fr>

Here is the debug output for

perl -wd  mcgui.pl in14_tut.instr

cheers. EF.

mica~farhi 55% mcgui.pl in14_tut.instr

Loading DB routines from perl5db.pl version 1.01
Emacs support available.

Enter h or `h h' for help.

Ambiguous use of expand => resolved to "expand" => at
/usr/ill/lib/perl5/site_pe
rl/Tk/Text.pm line 1038.
        require Tk/Text.pm called at (eval 5) line 2
        eval 'require Tk::Text
;' called at /usr/ill/perl/lib/base.pm line 36
        base::import('base', 'Tk::Text') called at
/usr/ill/lib/perl5/site_perl/
Tk/TextUndo.pm line 13
        Tk::TextUndo::BEGIN() called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm

line 1038
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1038
        require Tk/TextUndo.pm called at mcgui.pl line 12
        main::BEGIN() called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm line
103
8
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1038
Ambiguous use of expand => resolved to "expand" => at
/usr/ill/lib/perl5/site_pe
rl/Tk/Text.pm line 1075.
        require Tk/Text.pm called at (eval 5) line 2
        eval 'require Tk::Text
;' called at /usr/ill/perl/lib/base.pm line 36
        base::import('base', 'Tk::Text') called at
/usr/ill/lib/perl5/site_perl/
Tk/TextUndo.pm line 13
        Tk::TextUndo::BEGIN() called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm

line 1075
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1075
        require Tk/TextUndo.pm called at mcgui.pl line 12
        main::BEGIN() called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm line
107
5
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1075
main::(mcgui.pl:3):     if($ENV{"MCSTAS"}) {
  DB<1> r ******** Here is the program start ***********************
Signal SEGV at mcgui.pl line 375
        main::__ANON__() called at /usr/ill/perl/lib/perl5db.pl line 1136
        Tk::Widget::waitVariable('Tk::Toplevel=HASH(0x10c171a0)',
'SCALAR(0x106a
de78)') called at mcgui.pl line 380
        main::dialog_get_out_file('MainWindow=HASH(0x10abdacc)',
'in14_tut.instr
', 1) called at mcgui.pl line 416
        main::compile_instrument('MainWindow=HASH(0x10abdacc)', 1) called at
mcg
ui.pl line 436
        main::menu_compile('MainWindow=HASH(0x10abdacc)') called at mcgui.pl
lin
e 562
        main::__ANON__() called at /usr/ill/perl/lib/perl5db.pl line 1134
        eval {...} called at /usr/ill/perl/lib/perl5db.pl line 1134
        Tk::__ANON__('Tk::Menu=HASH(0x10b52674)', 'active') called at
/usr/ill/l
ib/perl5/site_perl/Tk/Menu.pm line 530
        Tk::Menu::Invoke('Tk::Menu=HASH(0x10b52674)', 1) called at
/usr/ill/perl
/lib/perl5db.pl line 1136
        eval {...} called at /usr/ill/perl/lib/perl5db.pl line 1136
        Tk::MainLoop() called at mcgui.pl line 745
Abort (core dumped)


--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue des Martyrs, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From ron at ill.fr  Wed Feb 16 18:30:23 2000
From: ron at ill.fr (Ron Ghosh)
Date: Wed, 16 Feb 2000 18:30:23 +0100
Subject: Bugs in McStas/McGUI-2
References: <01JLZ0W0AJMM91DJFO@risoe.dk>
Message-ID: <38AADEAF.333BE852@ill.fr>

I thought I was making some progress when I found that Emmanuel had
two components that weren't in the library, i.e. a manual compilation
using mcstas stopped at this first stage.  I quickly excised the two
modules, but then it still crashed, though the mcstas stage
window stayed up longer(!).   I then did a hand compile of the
c from mcstas, and it brought up a number of odd errors.  Perhaps
the SGI error returns are not treated well enough, and mcgui ploughs
on relentlessly and crashes.

It is too late for attachments - I'll simply copy in results:

Manual compilation of slightly hacked code (removing SOURCE and MON1D,
and replacing source by cold_guide at absolute 0,0,0)

----------------------------------------------------------------------
is1 95% /usr/ill/perl/bin/perl -d /usr/ill/bin/mcgui in14r.instr

Loading DB routines from perl5db.pl version 1.01
Emacs support available.

Enter h or `h h' for help.

Ambiguous use of expand => resolved to "expand" => at
/usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1038.
        require Tk/Text.pm called at (eval 5) line 2
        eval 'require Tk::Text
;' called at /usr/ill/perl/lib/base.pm line 36
        base::import('base', 'Tk::Text') called at
/usr/ill/lib/perl5/site_perl/Tk/TextUndo.pm line 13
        Tk::TextUndo::BEGIN() called at
/usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1038
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1038
        require Tk/TextUndo.pm called at /usr/ill/bin/mcgui line 12
        main::BEGIN() called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1038
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1038
Ambiguous use of expand => resolved to "expand" => at
/usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1075.
        require Tk/Text.pm called at (eval 5) line 2
        eval 'require Tk::Text
;' called at /usr/ill/perl/lib/base.pm line 36
        base::import('base', 'Tk::Text') called at
/usr/ill/lib/perl5/site_perl/Tk/TextUndo.pm line 13
        Tk::TextUndo::BEGIN() called at
/usr/ill/lib/perl5/site_perl/Tk/Text.pm line 1075
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1075
        require Tk/TextUndo.pm called at /usr/ill/bin/mcgui line 12
        main::BEGIN() called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1075
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1075
main::(/usr/ill/bin/mcgui:3):   if($ENV{"MCSTAS"}) {
  DB<1> r
Signal SEGV at /usr/ill/bin/mcgui line 375
        main::__ANON__() called at /usr/ill/perl/lib/perl5db.pl line
1136
        Tk::Widget::waitVariable('Tk::Toplevel=HASH(0x10c04110)',
'SCALAR(0x106a8f2c)') called at /usr/ill/bin/mcgui line 380
        main::dialog_get_out_file('MainWindow=HASH(0x10ab9b68)',
'in14r.instr', 1) called at /usr/ill/bin/mcgui line 416
        main::compile_instrument('MainWindow=HASH(0x10ab9b68)', 1)
called at /usr/ill/bin/mcgui line 436
        main::menu_compile('MainWindow=HASH(0x10ab9b68)') called at
/usr/ill/bin/mcgui line 562
        main::__ANON__() called at /usr/ill/perl/lib/perl5db.pl line
1134
        eval {...} called at /usr/ill/perl/lib/perl5db.pl line 1134
        Tk::__ANON__('Tk::Menu=HASH(0x10b3df28)', 'active') called at
/usr/ill/lib/perl5/site_perl/Tk/Menu.pm line 530
        Tk::Menu::Invoke('Tk::Menu=HASH(0x10b3df28)', 1) called at
/usr/ill/perl/lib/perl5db.pl line 1136
        eval {...} called at /usr/ill/perl/lib/perl5db.pl line 1136
        Tk::MainLoop() called at /usr/ill/bin/mcgui line 745
Abort (core dumped)


not really much help I'm afraid!  It just seems to be in the event loop.

-----------------------------------------------------------------------------
Is it because the compilation failed on the SGI?

is1 103% mcstas -o fff.c in14r.instr

is1 109% cc -c fff.c
cc-1174 cc: WARNING File = mcstas-r.c, Line = 153
  The variable "k" was declared but never referenced.

    int i,j, k;
             ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 460
  The variable "x" was declared but never referenced.

    double x,y,z;
           ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 460
  The variable "y" was declared but never referenced.

    double x,y,z;
             ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 460
  The variable "z" was declared but never referenced.

    double x,y,z;
               ^

cc-1552 cc: WARNING File = mcstas-r.c, Line = 962
  The variable "v" is set but never used.

    double v, D, t_in, t_out, y_in, y_out;
           ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 1073
  The variable "mcrt_v1x" was declared but never referenced.

    rotate(xt, yt, zt, xi, yi, zi, theta, nx, ny, nz);
    ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 1073
  The variable "mcrt_v1y" was declared but never referenced.

    rotate(xt, yt, zt, xi, yi, zi, theta, nx, ny, nz);
    ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 1073
  The variable "mcrt_v1z" was declared but never referenced.

    rotate(xt, yt, zt, xi, yi, zi, theta, nx, ny, nz);
    ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 1074
  The variable "mcrt_v1x" was declared but never referenced.

    rotate(*xo, *yo, *zo, xt, yt, zt, phi, xi, yi, zi);
    ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 1074
  The variable "mcrt_v1y" was declared but never referenced.

    rotate(*xo, *yo, *zo, xt, yt, zt, phi, xi, yi, zi);
    ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 1074
  The variable "mcrt_v1z" was declared but never referenced.

    rotate(*xo, *yo, *zo, xt, yt, zt, phi, xi, yi, zi);
    ^

cc-1174 cc: WARNING File = mcstas-r.c, Line = 1202
  The variable "pos" was declared but never referenced.

    int i, j, pos;
              ^

cc-1008 cc: ERROR File = in14r.instr, Line = 102
  A new-line character appears inside a string literal.

    printf("Incident Ki = %f Angs-1, Exchange Q=%f Angs-1, Final Kf = %f 
           ^

cc-1018 cc: ERROR File = in14r.instr, Line = 103
  An unmatched left parentheses "(" appears in an expression.

  Angs-1\n",Ki,Q,Kf);
  ^

cc-1007 cc: ERROR File = in14r.instr, Line = 103
  The indicated token is not valid in this context.

  Angs-1\n",Ki,Q,Kf);
        ^

cc-1008 cc: ERROR File = in14r.instr, Line = 103
  A new-line character appears inside a string literal.

  Angs-1\n",Ki,Q,Kf);
          ^

cc-1174 cc: WARNING File = fff, Line = 2206
  The variable "mctr2" was declared but never referenced.

      Rotation mctr1, mctr2;
                      ^

cc-1174 cc: WARNING File = /usr/ill/lib/mcstas/Guide.comp, Line = 45
  The variable "vlen2" was declared but never referenced.

    double vlen2,nlen2;                           /* Vector lengths
squared */
           ^

cc-1174 cc: WARNING File = /usr/ill/lib/mcstas/Guide.comp, Line = 50
  The variable "lwhalf" was declared but never referenced.

    double lwhalf = l*whalf, lhhalf = l*hhalf;
           ^

cc-1174 cc: WARNING File = /usr/ill/lib/mcstas/Guide.comp, Line = 50
  The variable "lhhalf" was declared but never referenced.

    double lwhalf = l*whalf, lhhalf = l*hhalf;
                             ^

cc-1174 cc: WARNING File = /usr/ill/lib/mcstas/Guide.comp, Line = 142
  The variable "x" was declared but never referenced.

    double x;
           ^

cc-1174 cc: WARNING File = /usr/ill/lib/mcstas/Guide.comp, Line = 143
  The variable "i" was declared but never referenced.

    int i;
        ^

4 errors detected in the compilation of "fff.c".
------------------------------------------------------------------------
I hope this might give some hint to you!

Bon soir,  Ron

-- 
Ron Ghosh, Institut Laue Langevin, B.P. 156    tel: +33-476207178
38042 Grenoble cedex 9, FRANCE                 fax: +33-476483906




From kristian.nielsen at risoe.dk  Thu Feb 17 10:32:31 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 17 Feb 2000 10:32:31 +0100
Subject: Bugs in McStas/McGUI-2
In-Reply-To: <38AADEAF.333BE852@ill.fr> (message from Ron Ghosh on Wed, 16 Feb
	2000 18:30:23 +0100)
Message-ID: <mailman.96.1511353198.451.mcstas-users@mailman2.mcstas.org>

Hi Ron and Emmanuel,

Thanks for the debug output. I took a look at them and have some ideas.

I think the most likely problem is that mcgui fails to start the
"mcstas" program. In that case the mcgui in v1.2 starts running two
processes simultaneously in Perl/Tk (due to a bug in mcgui). This
usually causes spectacular crashes.

I just tried running mcgui where I artificially made mcgui fail to spawn
mcstas, and got an error similar to what you reported. I fixed the bug
in mcgui, and the new version does not crash.

I put the new version of mcgui up on host "mica", in the directory
"/home/cs/nielsen/mcgui-crash" as the file "mcgui-new.pl". Please try
the new version, and see if it works any better. In any case, please
let me know how it works!

About the compilation problem with in14_tut.instr that Ron had: this is
caused by an error in the file; in line 102 there is a spurious newline
inside a string constant (as reported by the C compiler). I believe this
is unrelated to the mcgui problem. A fixed instrument file is found in
the same directory as the new mcgui.

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790





From ron at ill.fr  Thu Feb 17 16:50:19 2000
From: ron at ill.fr (Ron Ghosh)
Date: Thu, 17 Feb 2000 16:50:19 +0100
Subject: Bugs in McStas/McGUI-2
References: <01JM0EOI7MKE91D5Q7@risoe.dk>
Message-ID: <38AC18BB.6D9A81BB@ill.fr>

Thanks very much for your comments and corrections.  I shall be away
for a few days now, but Emmanuel hopes to find time tomorrow
to check out the changes.   As usual it is the error detection
that complicates programming, and we certainly can provide errors!
Best wishes, Ron.
-- 
Ron Ghosh, Institut Laue Langevin, B.P. 156    tel: +33-476207178
38042 Grenoble cedex 9, FRANCE                 fax: +33-476483906




From farhi at ill.fr  Thu Feb 17 19:36:54 2000
From: farhi at ill.fr (Farhi)
Date: Thu, 17 Feb 2000 19:36:54 +0100
Subject: mcgui-new
Message-ID: <38AC3FC6.942587D@ill.fr>

Hy Kristian,

I'm afraid it does not work better !!
I've tried to look inside mcgui.pl
It seems that that error occurs during the waitVariable call of the do
loop (function dialog_get_out_file)

do {
   $dlg->waitVariable(\$state);
      } until $state;

Here is the perldb output (which is about the same as before, I've added
some 'print breakpoints'...) :

mica~farhi 44% ./mcgui-new.pl in14_tut.instr

Loading DB routines from perl5db.pl version 1.01
Emacs support available.

Enter h or `h h' for help.

Ambiguous use of expand => resolved to "expand" => at
/usr/ill/lib/perl5/site_pe
rl/Tk/Text.pm line 1038.
        require Tk/Text.pm called at (eval 5) line 2
        eval 'require Tk::Text
;' called at /usr/ill/perl/lib/base.pm line 36
        base::import('base', 'Tk::Text') called at
/usr/ill/lib/perl5/site_perl/
Tk/TextUndo.pm line 13
        Tk::TextUndo::BEGIN() called at
/usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1038
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1038
        require Tk/TextUndo.pm called at ./mcgui-new.pl line 12
        main::BEGIN() called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 103
8
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1038
Ambiguous use of expand => resolved to "expand" => at
/usr/ill/lib/perl5/site_pe
rl/Tk/Text.pm line 1075.
        require Tk/Text.pm called at (eval 5) line 2
        eval 'require Tk::Text
;' called at /usr/ill/perl/lib/base.pm line 36
        base::import('base', 'Tk::Text') called at
/usr/ill/lib/perl5/site_perl/
Tk/TextUndo.pm line 13
        Tk::TextUndo::BEGIN() called at
/usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1075
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1075
        require Tk/TextUndo.pm called at ./mcgui-new.pl line 12
        main::BEGIN() called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 107
5
        eval {...} called at /usr/ill/lib/perl5/site_perl/Tk/Text.pm
line 1075
main::(./mcgui-new.pl:3):       if($ENV{"MCSTAS"}) {
  DB<1> r
after savefocus
before for
before get_out_file_next call
before run_dialog_popup call
before run_dialog_reader
after run_dialog_reader
after fileevent
before do waitVariable
Signal SEGV at ./mcgui-new.pl line 380
        main::__ANON__() called at /usr/ill/perl/lib/perl5db.pl line
1136
        Tk::Widget::waitVariable('Tk::Toplevel=HASH(0x10c19248)',
'SCALAR(0x106a
de78)') called at ./mcgui-new.pl line 388
        main::dialog_get_out_file('MainWindow=HASH(0x10ac44a4)',
'in14_tut.instr
', 1) called at ./mcgui-new.pl line 429
        main::compile_instrument('MainWindow=HASH(0x10ac44a4)', 1)
called at ./m
cgui-new.pl line 449
        main::menu_compile('MainWindow=HASH(0x10ac44a4)') called at
../mcgui-new.
pl line 578
        main::__ANON__() called at /usr/ill/perl/lib/perl5db.pl line
1134
        eval {...} called at /usr/ill/perl/lib/perl5db.pl line 1134
        Tk::__ANON__('Tk::Menu=HASH(0x10b2d450)', 'active') called at
/usr/ill/l
ib/perl5/site_perl/Tk/Menu.pm line 530
        Tk::Menu::Invoke('Tk::Menu=HASH(0x10b2d450)', 1) called at
/usr/ill/perl
/lib/perl5db.pl line 1136
        eval {...} called at /usr/ill/perl/lib/perl5db.pl line 1136
        Tk::MainLoop() called at ./mcgui-new.pl line 761
Abort (core dumped)

Cheers. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue des Martyrs, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From kristian.nielsen at risoe.dk  Wed Feb 23 09:08:08 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 23 Feb 2000 09:08:08 +0100
Subject: mcgui-new
In-Reply-To: <38AC3FC6.942587D@ill.fr> (message from Farhi on Thu, 17 Feb 2000
	19:36:54 +0100)
Message-ID: <mailman.97.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Thu, 17 Feb 2000 19:36:54 +0100
> From: Farhi <farhi at ill.fr>

> I'm afraid it does not work better !!

Ok, that is just the way it is then.

> I've tried to look inside mcgui.pl
> It seems that that error occurs during the waitVariable call of the do
> loop (function dialog_get_out_file)

Yes. I am pretty sure that the problem is a conflict between the main
mcgui process, the spawned compiler process, and the Tk/X Windows
System. I am not sure of the details though, so I would ask you to run
two more tests that will help to pinpoint the problem.

I have put two new version of mcgui on mica, in
~nielsen/mcgui-crash/. They are called mcgui-1.pl and mcgui-2.pl. They
are both identical to the previous mcgui except for the exec() call that
actually starts the mcstas compiler program.

Could you try running both of them and let me know the results? The
commands would be

    /usr/ill/perl/bin/perl -d mcgui-1.pl in14_tut.instr
    /usr/ill/perl/bin/perl -d mcgui-2.pl in14_tut.instr

and for each command, just select "File"->"Compile instrument".

I also did a web search, and for a similar problem it was suggested to
install a newer version of perl. Maybe Ron will want to try that at some
point.

The mcgui-1.pl starts a simple "echo" command instead of the McStas and
C compiler. On my machine, compilation emits two
"EXEC call succeeded ok" messages, and succeeds.

The mcgui-2.pl does not start any commands at all. On my machine,
compilation fails with "Error: exec() of mcstas failed!" and two curious
"Callback called exit." messages.

 - Kristian.





From farhi at ill.fr  Wed Feb 23 09:33:12 2000
From: farhi at ill.fr (Farhi)
Date: Wed, 23 Feb 2000 09:33:12 +0100
Subject: mcgui tests and more
Message-ID: <38B39B48.CFA9AF74@ill.fr>

Hy Kristian,

the mcgui saga goes on.
I've tested the two versions
1- mcgui-1.pl : crash, here if the trace output
  DB<1> r
Signal SEGV at mcgui-1.pl line 375
        main::__ANON__() called at /usr/ill/perl/lib/perl5db.pl line
1136
        Tk::Widget::waitVariable('Tk::Toplevel=HASH(0x10c18260)',
'SCALAR(0x106ade78)') called at mcgui-1.pl line 380
        main::dialog_get_out_file('MainWindow=HASH(0x10abeba4)',
'in14_tut.instr', 1) called at mcgui-1.pl line 419
        main::compile_instrument('MainWindow=HASH(0x10abeba4)', 1)
called at mcgui-1.pl line 439
        main::menu_compile('MainWindow=HASH(0x10abeba4)') called at
mcgui-1.pl line 568
        main::__ANON__() called at /usr/ill/perl/lib/perl5db.pl line
1134
        eval {...} called at /usr/ill/perl/lib/perl5db.pl line 1134
        Tk::__ANON__('Tk::Menu=HASH(0x10b53f4c)', 'active') called at
/usr/ill/lib/perl5/site_perl/Tk/Menu.pm line 530
        Tk::Menu::Invoke('Tk::Menu=HASH(0x10b53f4c)', 1) called at
/usr/ill/perl/lib/perl5db.pl line 1136
        eval {...} called at /usr/ill/perl/lib/perl5db.pl line 1136
        Tk::MainLoop() called at mcgui-1.pl line 751
Abort (core dumped)
2- mcgui-2.pl : cannot fork
  DB<1> r
DB::fake::(/usr/ill/perl/lib/perl5db.pl:2083):
2083:     "Debugged program terminated.  Use `q' to quit or `R' to
restart.";
Forked, but do not know how to change a TTY.
Define $DB::fork_TTY or get_fork_TTY().

I'm now finisshing a general Monitor component. It can handle any kind
of output (0D, 1D and 2D, and multiple 1D output), with 'intelligent'
features when they are not provided by user. This should avoid people
from writing dozens of monitors on the same model. I tell you when I
incorporate it to the unofficial components and automatic web page. This
latter works ok, but can you also sort components by category in the
list ?

Cheers. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue des Martyrs, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From kristian.nielsen at risoe.dk  Wed Feb 23 10:06:24 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 23 Feb 2000 10:06:24 +0100
Subject: mcgui tests and more
In-Reply-To: <38B39B48.CFA9AF74@ill.fr> (message from Farhi on Wed, 23 Feb
	2000 09:33:12 +0100)
Message-ID: <mailman.98.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Wed, 23 Feb 2000 09:33:12 +0100
> From: Farhi <farhi at ill.fr>

> I've tested the two versions
> 1- mcgui-1.pl : crash, here if the trace output
> 2- mcgui-2.pl : cannot fork

Ok, thanks for the information. It seems pretty clear that the problem
is that when another program is called (whether the mcstas compiler or a
simple echo), it causes a conflict with the Tk/X connection. The "cannot
fork" is just the Perl debugger; could you should try mcgui-2.pl without
the debugger and see if it crashes? If possible, we should also try with
a newer version of Perl, though that will probably mean a lot of work
for Ron. I will think some more about the problem and maybe ask on the
Perl/Tk mailing list.

> I'm now finisshing a general Monitor component. It can handle any kind
> of output (0D, 1D and 2D, and multiple 1D output), with 'intelligent'
> features when they are not provided by user. This should avoid people
> from writing dozens of monitors on the same model. I tell you when I

Sounds very good! A solution to the  "dozens of monitors" problem would
be very nice indeed!

> incorporate it to the unofficial components and automatic web page. This
> latter works ok, but can you also sort components by category in the
> list ?

In fact, I already did :-)

    http://neutron.risoe.dk/mcstas/mcdoc/test/

My development version of McStas also uses subdirectories for components
as you suggested. I also have default values for component parameters
and instrument parameters that have string values.

 - Kristian.





From farhi at ill.fr  Wed Feb 23 10:24:35 2000
From: farhi at ill.fr (Farhi)
Date: Wed, 23 Feb 2000 10:24:35 +0100
Subject: mcgui tests and more
References: <01JM8RI8DXZ68WW9ML@risoe.dk>
Message-ID: <38B3A753.BCC1C0EB@ill.fr>

The mcgui-2 still crashes. But anyway, it's strange to see mcgui crash on SGI
but not on Linux...

On mica/SGI/IRIX : This is perl, version 5.005_02 built for -irix
on tequila/Linux/i586 : This is perl, version 5.005_03 built for i586-linux
on macfarhi/Linux/ppc : This is perl, version 5.005_03 built for ppc-linux

Perhaps the _03 is better...

Thanks pal.
EF.

Kristian Nielsen wrote:

> > Date: Wed, 23 Feb 2000 09:33:12 +0100
> > From: Farhi <farhi at ill.fr>
>
> > I've tested the two versions
> > 1- mcgui-1.pl : crash, here if the trace output
> > 2- mcgui-2.pl : cannot fork
>
> Ok, thanks for the information. It seems pretty clear that the problem
> is that when another program is called (whether the mcstas compiler or a
> simple echo), it causes a conflict with the Tk/X connection. The "cannot
> fork" is just the Perl debugger; could you should try mcgui-2.pl without
> the debugger and see if it crashes? If possible, we should also try with
> a newer version of Perl, though that will probably mean a lot of work
> for Ron. I will think some more about the problem and maybe ask on the
> Perl/Tk mailing list.
>
> > I'm now finisshing a general Monitor component. It can handle any kind
> > of output (0D, 1D and 2D, and multiple 1D output), with 'intelligent'
> > features when they are not provided by user. This should avoid people
> > from writing dozens of monitors on the same model. I tell you when I
>
> Sounds very good! A solution to the  "dozens of monitors" problem would
> be very nice indeed!
>
> > incorporate it to the unofficial components and automatic web page. This
> > latter works ok, but can you also sort components by category in the
> > list ?
>
> In fact, I already did :-)
>
>     http://neutron.risoe.dk/mcstas/mcdoc/test/
>
> My development version of McStas also uses subdirectories for components
> as you suggested. I also have default values for component parameters
> and instrument parameters that have string values.
>
>  - Kristian.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue des Martyrs, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From kristian.nielsen at risoe.dk  Wed Feb 23 10:50:22 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 23 Feb 2000 10:50:22 +0100
Subject: mcgui tests and more
In-Reply-To: <38B3A753.BCC1C0EB@ill.fr> (message from Farhi on Wed, 23 Feb
	2000 10:24:35 +0100)
Message-ID: <mailman.99.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Wed, 23 Feb 2000 10:24:35 +0100
> From: Farhi <farhi at ill.fr>

> The mcgui-2 still crashes. But anyway, it's strange to see mcgui crash on SGI

I see, that is surprising ... I will look into it.

> On mica/SGI/IRIX : This is perl, version 5.005_02 built for -irix

Hm, this is quite strange. When I log into mica, I get

    mica 3% /usr/ill/perl/bin/perl -v
    This is perl, version 5.004_04 built for IP22-irix
    mica 2% /usr/sbin/perl -v
    This is perl, version 5.004_04 built for irix-n32

Where is the Perl 5.005_02 on mica?

I am starting to suspect that the problem may be caused by the mixing of
different perl versions on mica. Mixing different versions is a sure way
to get in trouble with Perl, in my experience...

 - Kristian.





From kristian.nielsen at risoe.dk  Wed Feb 23 11:17:52 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 23 Feb 2000 11:17:52 +0100
Subject: Investigating mcgui crash on mica
Message-ID: <mailman.100.1511353198.451.mcstas-users@mailman2.mcstas.org>

Hi Emmanuel,

Ok, I will start investigating the problem in more detail. I plan to use
the X server on macfarhi to display the Tk stuff on (I will write some
simple test programs that will not need any input!). I will try not to
disturb anything on the screen, but if strange windows start to pop up,
I am probably the one causing it. If it causes any trouble for you let
me know, and I will think of something else to try.

 - Kristian.





From farhi at ill.fr  Thu Feb 24 20:37:58 2000
From: farhi at ill.fr (Farhi)
Date: Thu, 24 Feb 2000 20:37:58 +0100
Subject: mcdoc
References: <01JLPGSZB0BU91BJNC@risoe.dk>
Message-ID: <38B58896.87DB233D@ill.fr>


Hy Kristian,

I've just finished my general monitor. It seems that it can handle any set of
1D monitors at the same position, as well as a 2D monitor, and at the samme
time a neutron variable list (such as the one produced by my old kw_monitor).
All current monitors appear obsolete , except 3D if some exist !, or special
ones (some exotic variables).
It handles many options, default values, and automatic limits... I've started
to test it, and it's ok for 0D, multiple 1D at the same place, list of
neutrons (such as kw_monitor), 2D monitors, and mixtures of all this !

About mcdoc:
1- it's great (subdirectories, history, links...)
2- I've seen that there are default vaules, sub directories, optional
parameters. great
3- you should add a line in index.html saying what is a bold component vs a
normal font one
4- I usually define lots of OUTPUT parameters, in order not to mix them with
possible other variables from other components. This produces a long list of
output parameters. I think it's better to move the in/out param sections at
the end of the page
5- It could be fine to set tags (<a name=>) and a short (1 line centered)
table of contents at the begining of html description
6- in mcstas DETECTOR_OUT... functions, also print out the name of output
file after Detector:.... [filename]

Now how should we share the two pages ? I make a tar of my components and
send it to you by mail, and you do the same ?

I think a go home now (it's sure time !!)

EF.

Kristian Nielsen wrote:

> Hi Emmanuel,
>
> I was much inspired by our discussion of the automatic generation of
> documentation (web pages, ...) from the header comments in components. I
> now have a first working version, and I hope we can work together on
> developing it.
>
> First, to see the results go to
>
>     http://neutron.risoe.dk/mcstas/mcdoc/test/
>
> These pages were generated automatically by McDoc from the component
> sources. The Perl program McDoc itself is found at
>
>     http://neutron.risoe.dk/mcstas/mcdoc/test/mcdoc.pl
>
> To generate a set of web pages, you copy the component source codes into
> a directory and issue the command
>
>     perl mcdoc.pl *.comp
>
> Components can also be placed in subdirectories, as seen on the
> demonstration pages, using a command like
>
>     perl mcdoc.pl */*.comp
>
> The comment syntax uses %IDENTIFICATION, %DESCRIPTION, %PARAMETERS, and
> %END keywords to mark the different sections; keywords may be
> %abbreviated.
>
>  * In the identification section, "author:" (or "written by" for backwards
> compatibility) denote author; "date:", "version:", and "origin:" are
> also supported. These must be on a single line. Everything else is part
> of the "short description" of the component.
>
>  * In the parameters section, descriptions have the form
> "name: [unit] text" or "name: text [unit]". These may span multiple
> lines; subsequent lines must be indented by at least four spaces. Note
> that square brackets [] should be used for units. Normal parenthesis are
> also supported for backwards compatibility, but nested parenthesis do
> not work well.
>
>  * The description section contains text in free format.
>
>  * After %END, no more header text is parsed.
>
> I also have an idea for how we can cooperate on maintaining the
> component library. We need to have each a master directory containing
> the components that each of us maintain. For each web server mirror,
> every night (or however often), an automatic job copies the contents of
> both master directory into a single directory on the web server and runs
> the mcdoc.pl script on the contents. This way, either of us can update
> our private master directory individually and the change will be
> reflected on both the Ris? and ILL pages.
>
> So, what do you think? I suggest you try to convert the headers of a few
> of your own components and see how it works out. You will probably have
> some suggestions for me about how to improve the header syntax. Once we
> have a good agreement on the syntax, we can start rewriting all the
> headers in the library (I suggest that I handle the 39 components that
> are part of the official v1.2 release and you handle the rest of the
> components on the ILL page).
>
> I also have other plans for how to extend mcdoc. The documentation could
> be made accessible from within the graphical user interface. The
> web-pages should have links to postscript files of the individual
> section in the McStas manual where relevant. And it should be possible
> to put in pictures and links to other web pages (sample instrument for
> example) in a %LINKS section in the header.
>
>  - Kristian.
>
> --
> Kristian Nielsen        kristian.nielsen at risoe.dk
> Ris? National Laboratory
> Condensed Matter Physics and Chemistry Department
> Tel. +45 4677 5515   Fax +45 4677 4790

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue des Martyrs, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94





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From farhi at ill.fr  Tue Feb 29 17:04:34 2000
From: farhi at ill.fr (Farhi)
Date: Tue, 29 Feb 2000 17:04:34 +0100
Subject: Update of Web site
Message-ID: <38BBEE12.AA60C542@ill.fr>

Hy Kristian,

I've updated the ILL web site, to point to your official components
page, and to my reduced unofficial web page.
You will see there the Monitor_nD, which replaces all other existing
monitors easely.

For instance (I just put the option string)
"energy" is equivalent to E_monitor
"x y" is equivalent to PSD_monitor
"theta phi" is a PSD_4PI
"list all neutrons kx ky kz energy" is a dump of all passing neutrons
(k,w)
you can also use 4 shapes for detector, as well as many options.

Automatic page is at
<http://www.ill.fr/tas/mcstas/components/monitors/Monitor_nD.html>

Cheers. EF.

NB : Ron will re-install all perl stuff on SGI/IRIX next week perhaps...



--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue J. Horowitz, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From hansen at ill.fr  Thu Feb 24 11:22:21 2000
From: hansen at ill.fr (Thomas C Hansen)
Date: Thu, 24 Feb 2000 11:22:21 +0100
Subject: Suggestions for McStas
Message-ID: <38B50658.6B5F6693@ill.fr>

Dear Kristian,

McStas 1.2 works fine, thanks for all your work. However, I've got some
(disordered) suggestions for amelioration, as you asked for it.

1. Having DEFINITION PARAMETERS (so strings, etc.) also for the INSRument, not
only for the COMPonent would be fine.

2. The 'make' functionality of mcrun and mcgui is limited to the *.instr file.
It would be great, if these front ends could check as well for invoked *.comp
and force recompiling if these are newer than *.out and *.c.

3. The trace (mcdisplay) option in mcgui should accept options like --multi and
--inspect.

4. The circle in MCDISPLAY draws only a rough polygon. that's okay for small
circles, but if I present my curved 1D PSD, having a radius of about 1.5 meters,
I cannot see precisely enough the neutron's trajectory in the detection gap.
That's not really a problem for me, as I can work around with some hundred short
lines on a circle (permitting as well to draw only a part of a circle), but
maybe for others ...

5. The Beamstop_rectangular component draws very funny lines with mcdisplay.

6. It would be a great job (a lot of work), but really useful, to have some kind
of a standard adaptation procedure/macro/subroutine also for other components
than the source, as well the possibility to invoke it into new/modified
components in a standardized way. I am thinking for instance of targeting in
monochromator crystals (e.g. for the vertical divergence a MC choice of phi is
done which could result in neutrons never hitting neither sample or detector),
or the implementation of a complex powder sample with several Bragg reflections,
incoherent scattering, multiple scattering, etc. could become more efficient and
maybe easier.

Good luck, and thanks again,

Thomas

--
Dr. Thomas C HANSEN, Instrument Scientist D20, Diffraction Group
Institut Max von Laue-Paul Langevin, BP 156, 38042 Grenoble C?dex 9, France
ILL4-1st floor room 100, Phone +33(0)476207044, Fax +33(0)476207648
mailto:hansen at ill.fr, http://www.ill.fr/YellowBook/D20
Private: 13, all?e des ?tangs, 38240 Meylan, France, +33(0)476180553








From kristian.nielsen at risoe.dk  Mon Mar  6 13:42:23 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: Mon, 06 Mar 2000 13:42:23 +0100
Subject: New on-line component documentation for McStas
Message-ID: <01JMPQK3J2NK8X0Q6T@risoe.dk>

Dear all McStas users,

A new set of web pages containing documentation of the component library
have been installed on the McStas web pages at

    http://neutron.risoe.dk/mcstas/mcdoc/components/

These pages are generated automatically by a program called McDoc from
component sources at both Risoe and ILL and thus have a much better
chance of being up-to-date than the previous manually built on-line
documentation. I hope that they will prove useful to users of McStas.

It is fairly easy to add your own components into this system. See the
documentation at

    http://neutron.risoe.dk/mcstas/mcdoc/

for details.

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790
Encryption PGP key http://neutron.risoe.dk/kn.txt




From farhi at ill.fr  Tue Mar  7 17:32:31 2000
From: farhi at ill.fr (Farhi)
Date: Tue, 07 Mar 2000 17:32:31 +0100
Subject: New tested components for McStas
Message-ID: <38C52F1E.E5C40370@ill.fr>

Hello McStas users,

I here annouce 3 new / updated components for McStas. These are
available at

< http://neutron.risoe.dk/mcstas/mcdoc/components/ >

and

< http://www.ill.fr/tas/mcstas/components/ >

1-The Source_Optimizer (v 0.07) is a component that optimizes the McStas
neutron shots in order to reach a given place in the simulation. These
places (you should even be able to use more that one) are indicated by
the Monitor_Optimizer positions.
The Source_Optimizer only requires 1 parameter (it acts on the whole
neutron beam) that is a string, and can be empty.
This 'options' parameter is parsed, and can contain some user choices
concerning the optimization process, specified with flexible keywords.
I personnally use : options = "", that is the default configuration.
This component is 'intelligent' and can adapt it's features to your
simulation. The optimization is made on neutron variables x y vx vy vz,
considered to be independent. The energy distribution is kept, as far as
possible. The flux is kept of course.
The speedup on neutron counts reaching monitors  is at least of 20. I
just obtained 50 in my last test !

(near the source, at a distance of 1 mm in my tests)
COMPONENT optim_s = Source_Optimizer(
    options="")

2- The Monitor_Optimizer (v 0.07) works with the Source_Optimizer. It
only requires x/y dimension (4 parameters)

(near the optimisation point, usually sample or detector)
COMPONENT optim_m = Monitor_Optimizer(
    xmin = -0.05, xmax = 0.05,
    ymin = -0.05, ymax = 0.05)

3- The Monitor_nD (v 0.13) is a general monitor that can act as any of
all previous monitors. It only requires dimension (4 params in x/y
size), and an 'options' string specifying what to monitor.
This 'options' parameter is parsed, and can contain some user choices
concerning the monitor. A 0D monitor is default (just flux).
There are 25 variables available for monitoring (wavevector, speed,
position, divergences, etc...), and you can decide to output these as 1D
or 2D (related variables) signals. A log (list) of neutron variables is
also possible ('list all neutrons' or 'list 1000 neutrons' options).
A special 'auto limits' feature compute what are the necessary limits
for the monitor.
The shape of the monitor can be plane square, disk, sphere and cylinder.

I just recorded a kz_kx image of neutron beam at sample position with

(this one is just after the Monitor_Optimizer up-there, near my sample
position, at a distance of 1 mm)
COMPONENT MSample = Monitor_nD(
     xmin = -0.05, xmax = 0.05,
     ymin = -0.05, ymax = 0.05,
     options = "kx kz, all bins = 50, auto limits, file=MSample")

I hope that these components will be usefull to you, and don't hesitate
to contact me in case of questions, bugs, etc...

Cheers. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue J. Horowitz, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From poehlman at ill.fr  Wed Mar  1 14:13:55 2000
From: poehlman at ill.fr (Markus Poehlmann)
Date: Wed, 01 Mar 2000 14:13:55 +0100
Subject: IN6 simulation
Message-ID: <38BD1793.FA771D0C@ill.fr>

Dear Kristian Nielsen,

we want to simultate a Time of Flight instrument (ILL IN6) with the
McStas program. For our 3 monochromators (one behind another) we would
need a component that allows it for each neutron either to be propagated
(in the original z direction) or to be scattered independently.
Obviously this is not possible with the McStas monochromator component.
Do you have any idea of what we would have to change in the original
component ?
Thank you for your help.
Sincerely

Markus Poehlmann

For a better understanding of the problem, plaese see the picture:
http://www.ill.fr/YellowBook/IN6/
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From kristian.nielsen at risoe.dk  Wed Mar  1 14:53:47 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 1 Mar 2000 14:53:47 +0100
Subject: IN6 simulation
In-Reply-To: <38BD1793.FA771D0C@ill.fr> (message from Markus Poehlmann on Wed,
	01 Mar 2000 14:13:55 +0100)
Message-ID: <mailman.101.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Wed, 01 Mar 2000 14:13:55 +0100
> From: Markus Poehlmann <poehlman at ill.fr>

> Dear Kristian Nielsen,
> 
> we want to simultate a Time of Flight instrument (ILL IN6) with the
> McStas program. For our 3 monochromators (one behind another) we would
> need a component that allows it for each neutron either to be propagated
> (in the original z direction) or to be scattered independently.
> Obviously this is not possible with the McStas monochromator component.

I would suggest that you use the Mosaic_anisotropic component. This
component is available in the new version 1.2 of McStas, which I believe
is already installed at the ILL. It is a direct replacement of the old
Monochromator component (same parameters), but it correctly handles many
more non-standard configurations, including a transmission configuration
like yours.

See the manual for further details, or just ask again if you have any
further questions.

Good luck!

 - Kristian.





From kristian.nielsen at risoe.dk  Fri Mar  3 11:27:43 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 3 Mar 2000 11:27:43 +0100
Subject: mcdoc
In-Reply-To: <38B58896.87DB233D@ill.fr> (message from Farhi on Thu, 24 Feb
	2000 20:37:58 +0100)
Message-ID: <mailman.102.1511353198.451.mcstas-users@mailman2.mcstas.org>

Hi Emmanuel,

Thanks for the comments. They were as always very useful, and I have
implemented all of them now (if you find something missing, please let
me know).

Your generic monitor is very interesting, and I am sure that it will
prove very useful. I am really hoping that you will write some
documentation in the same style as all the official components in the
McStas manual, so that I can include it in the next official
release. You do not have to use LaTeX, I will convert it for you from
whatever format you prefer to use.

I have also implemented a method for sharing our component libraries. We
need to set up a special directory on a web server at each institute
participating (currently only Ris? and ILL). This directory contains
ONLY the source code for the components to be shared (ie. my directory
contains the official components, your directory contains the rest). I
have written a small shell script,

    http://neutron.risoe.dk/mcstas/support/farhi/builddocs.sh

This script automatically downloads the component source codes from each
web server into common subdirectories. It then downloads the newest
mcdoc program from the Ris? server and re-builds all the documentation.

On mica, I have set up a demonstration in the /home/cs/nielsen/mcdoc/
directory. The command

    ./builddocs.sh

will download all components and build the web pages. Because of the
firewall, it is necessary to first execute

    setenv http_proxy proxy.ill.fr:8888

What you need to do is to set up a directory on your web server and keep
it updated with the newest source codes for the components you want to
share. Then we can both use the builddocs.sh script to create a single
component page with all components that are automatically kept
synchronized. What do you think?

Finally, with regard to the mcgui crash on SGI. From yours and Ron's
emails, I got the impression that this problem was solved with the new
Perl installation, is this correct?

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790
Encryption PGP key http://neutron.risoe.dk/kn.txt





From poehlman at ill.fr  Thu Mar  2 17:56:58 2000
From: poehlman at ill.fr (Markus Poehlmann)
Date: Thu, 02 Mar 2000 17:56:58 +0100
Subject: IN6 monochromator
Message-ID: <38BE9D5A.D3A4FC1A@ill.fr>

Dear Kristian Nielsen,

Thank you very much for your recent e-mail, but we think there is no
other way than to write an entirely new component. The problem is that
in our case we cannot calculate with weight factors because in a
bifurcation problem a neutron is either scattered or propagated
unscattered. But in the semiclassical approach like in McStas the
propagation probability is expressed by a weight factor.
So what we would need is a M o n t e C a r l o choice between scattering
and unscattered propagation. Could you please tell us how it would be
possible to introduce something like this in our new monochromator
component. Is there any C code or component available  that tackles that
problem? What e.g. does randnorm() exactly do?
Thank you for your help


Markus Poehlmann

P.S.: May be you could discuss that that directly with Helmut Schober on
the phone (+33 4 76 20 73 96)
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From kristian.nielsen at risoe.dk  Fri Mar  3 12:58:05 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 3 Mar 2000 12:58:05 +0100
Subject: IN6 monochromator
In-Reply-To: <38BE9D5A.D3A4FC1A@ill.fr> (message from Markus Poehlmann on Thu,
	02 Mar 2000 17:56:58 +0100)
Message-ID: <mailman.103.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Thu, 02 Mar 2000 17:56:58 +0100
> From: Markus Poehlmann <poehlman at ill.fr>

> So what we would need is a M o n t e C a r l o choice between scattering
> and unscattered propagation. Could you please tell us how it would be

This is exactly what the Mosaic_anisotropic component does. It computes
the scattering probability for the given incoming neutron and makes a
Monte Carlo choice between scattering or transmitting with this
probability. See the manual for McStas v1.2 page 59.

I think an example may be appropriate. I have written a simple
instrument with three monochromators in a neutron beam, each one
focusing at a different angle (88, 90, and 92 degrees) onto a
detector. See

    http://neutron.risoe.dk/mcstas/support/poehlman/mono_test.html

I hope this will get you started, otherwise just ask again, or phone me
on the number below.

> problem? What e.g. does randnorm() exactly do?

It returns a random number from a normal distribution with mean zero and
std. deviation 1. See manual page 82.

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790
Encryption PGP key http://neutron.risoe.dk/kn.txt





From kristian.nielsen at risoe.dk  Fri Mar  3 13:17:34 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 3 Mar 2000 13:17:34 +0100
Subject: Suggestions for McStas
In-Reply-To: <38B50658.6B5F6693@ill.fr> (message from Thomas C Hansen on Thu,
	24 Feb 2000 11:22:21 +0100)
Message-ID: <mailman.104.1511353198.451.mcstas-users@mailman2.mcstas.org>

Dear Thomas,

Thanks for your comments on McStas, they are most useful. I have already
implemented strings and integers as instrument parameters in my current
development version. I can send you a beta if you want, or you can wait
for the next version if you prefer (maybe a few months?).

I am not sure about the problems you mentioned with Beamstop_rectangular
and mcdisplay, do you have an example that you can send me where the
problem appears?

I agree that it would be good to generalize the adaption algorithm for
use in other components, and this is something I plan to do. I consider
the adaptive source a first prototype that will enable us to learn more
about how adaption can be used in practice, I have found it to be
surprisingly complex to get right.

The improved "make" and mcdisplay functionality in mcgui will probably
be implemented at some point it the not too-distant future.

Thanks again,

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790
Encryption PGP key http://neutron.risoe.dk/kn.txt





From hansen at ill.fr  Fri Mar  3 14:28:30 2000
From: hansen at ill.fr (Thomas C Hansen)
Date: Fri, 03 Mar 2000 14:28:30 +0100
Subject: Suggestions for McStas
References: <01JMLITBTW4M8WZOBD@risoe.dk>
Message-ID: <38BFBDFE.A4288961@ill.fr>

Kristian Nielsen wrote:

> Thanks for your comments on McStas, they are most useful. I have already
> implemented strings and integers as instrument parameters in my current
> development version. I can send you a beta if you want, or you can wait
> for the next version if you prefer (maybe a few months?).

For the moment I shall wait, I may contact you again, if I really ready to test
a new beta ersion.

> I am not sure about the problems you mentioned with Beamstop_rectangular
> and mcdisplay, do you have an example that you can send me where the
> problem appears?

I'll have a look again ...

> I agree that it would be good to generalize the adaption algorithm for
> use in other components, and this is something I plan to do. I consider
> the adaptive source a first prototype that will enable us to learn more
> about how adaption can be used in practice, I have found it to be
> surprisingly complex to get right.

Oh yes, it is complex ... setting N_xdiv and N_xpos to 1 and setting N_E to
something around 70 brought something completely spiky to something reasonable
.... The simulation is learning all the time, it could be usefull to write out a
certain distribution as a file, and use this file as an optional input for a
next simulation with similar (not necessary equal - as the distribution eolutes)
configuration.

Regards,

Thomas

--
Dr. Thomas C HANSEN, Instrument Scientist D20, Diffraction Group
Institut Max von Laue-Paul Langevin, BP 156, 38042 Grenoble C?dex 9, France
ILL4-1st floor room 100, Phone +33(0)476207044, Fax +33(0)476207648
mailto:hansen at ill.fr, http://www.ill.fr/YellowBook/D20
Private: 13, all?e des ?tangs, 38240 Meylan, France, +33(0)476180553







From poehlman at ill.fr  Fri Mar  3 15:00:21 2000
From: poehlman at ill.fr (Markus Poehlmann)
Date: Fri, 03 Mar 2000 15:00:21 +0100
Subject: IN6 monochromator
References: <01JMLI55B8K28WZOBD@risoe.dk>
Message-ID: <38BFC575.8C4A5C97@ill.fr>

Thank you very much for your reply and for the example instrument. The reason
why I asked you once more was that we have no one mono crystal monochromator
but 3 curved monochromators each consisting of 7 mono crystals. What I wanted
to do was to introduce a Monte Carlo choice in the curved monochromator
component (Mon2_foc) written by Peter Link.
I think for a further proceeding there are now 2 possible ways: Either to
introduce the Monte Carlo Choice in Mon2_foc or to modify the
Mosaic-anisotropic component in a way that there are 7 mono crystals instead
of one.
I will try both of them.
Unfortunately we had only the McStas 1.1 manual so that I could not find
these things like randnorm().

Markus Poehlmann

Kristian Nielsen wrote:

> > Date: Thu, 02 Mar 2000 17:56:58 +0100
> > From: Markus Poehlmann <poehlman at ill.fr>
>
> > So what we would need is a M o n t e C a r l o choice between scattering
> > and unscattered propagation. Could you please tell us how it would be
>
> This is exactly what the Mosaic_anisotropic component does. It computes
> the scattering probability for the given incoming neutron and makes a
> Monte Carlo choice between scattering or transmitting with this
> probability. See the manual for McStas v1.2 page 59.
>
> I think an example may be appropriate. I have written a simple
> instrument with three monochromators in a neutron beam, each one
> focusing at a different angle (88, 90, and 92 degrees) onto a
> detector. See
>
>     http://neutron.risoe.dk/mcstas/support/poehlman/mono_test.html
>
> I hope this will get you started, otherwise just ask again, or phone me
> on the number below.
>
> > problem? What e.g. does randnorm() exactly do?
>
> It returns a random number from a normal distribution with mean zero and
> std. deviation 1. See manual page 82.
>
>  - Kristian.
>
> --
> Kristian Nielsen        kristian.nielsen at risoe.dk
> Ris? National Laboratory
> Condensed Matter Physics and Chemistry Department
> Tel. +45 4677 5515   Fax +45 4677 4790
> Encryption PGP key http://neutron.risoe.dk/kn.txt

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From kristian.nielsen at risoe.dk  Mon Mar  6 10:29:36 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 6 Mar 2000 10:29:36 +0100
Subject: IN6 monochromator
In-Reply-To: <38BFC575.8C4A5C97@ill.fr> (message from Markus Poehlmann on Fri,
	03 Mar 2000 15:00:21 +0100)
Message-ID: <mailman.105.1511353198.451.mcstas-users@mailman2.mcstas.org>

I think you have actually three possibilities:

1. If your real monochromators are build each from 7 flat pieces,
consider using 3 x 7 instances of Mosaic_anisotropic in the
simulation. See the TAS1 example in the McStas manual for how to build a
simulation for a composit monochromator.

2. To extend Mon2_foc to do an MC choice should be straightforward. I
have not studied Peter Link's code in detail, but I think the relevant
sequence is

      tmp3 = (theta-theta0)/(MIN2RAD*mosaich);
      if(tmp3 > DIV_CUTOFF)
      {
        x = old_x; y = old_y; z = old_z; t = old_t;
      }
      else
      {
        p *= r0*exp(-tmp3*tmp3*4*log(2)); /* Use mosaics */

Here the weight is adjusted with the reflectivity
R=r0*exp(-tmp3*tmp3*4*log(2)). To instead do an MC choice, something
like the following should be used

      tmp3 = (theta-theta0)/(MIN2RAD*mosaich);
      if(tmp3 > DIV_CUTOFF || rand01() > r0*exp(-tmp3*tmp3*4*log(2)))
      {  /* No scattering */
        x = old_x; y = old_y; z = old_z; t = old_t;
      }
      else
      { /* Scatter, no weight adjustment here! */

I have not tested this, but the main point is to replace the weight
adjustment by the MC choice

    rand01() > r0*exp(-tmp3*tmp3*4*log(2))

3. To extend Mosaic_anisotropic to use a curved surface would also be
feasible, the only problem should be the need to understand the code of
both components. Only the geometry calculations should change, ie. the
computation of the intersection between the neutron flight path and the
monochromator surface, and the calculation of the surface normal.

Hope this helps,

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790
Encryption PGP key http://neutron.risoe.dk/kn.txt





From schober at ill.fr  Mon Mar  6 09:56:58 2000
From: schober at ill.fr (Helmut Schober)
Date: Mon, 06 Mar 2000 10:56:58 +0200
Subject: IN6 simulation
In-Reply-To: <01JMPJT511HE8WZ4JF@risoe.dk>
References: <38BFC575.8C4A5C97@ill.fr>
 (message from Markus Poehlmann on Fri, 03 Mar 2000 15:00:21 +0100)
Message-ID: <l03110702b4e920c13d18@[194.57.220.22]>

Dear Kristian,

    As the ILL contact responsible for the simulation of IN6, I would like
to thank you very much for the quick answers to Markus Poehlmann's
questions. We are new users of the simulation package and have to learn its
philosophy and use little by little . After discussion with Marcus this
morning we will probably opt for using several monochromator components.
That is what we had started out with but I guess due to a wrong use of the
arm component we forced the neutrons from one plate to the next, which
naturally left practically none in the detector. We learn the hard way. I
should spend more time on reading the manual. but unfortunatelly I am tied
up with many other duties so that Marcus does nearly all of the work. As he
does it very well I am optimistic that we will have a running simulation of
IN6 by the end of his 3 month stay at the ILL.

Thank you again for your help,

Helmut Schober

H. Schober
Institut Laue-Langevin
6 rue Jules Horowitz
BP 156
38042 Grenoble Cedex 9
Phone: + 33 4 76 20 73 96
Fax:     + 33 4 76 48 39 06






From farhi at ill.fr  Fri Mar  3 11:44:47 2000
From: farhi at ill.fr (Farhi)
Date: Fri, 03 Mar 2000 11:44:47 +0100
Subject: mcdoc
References: <01JMLEZ4T6UU8WZSGK@risoe.dk>
Message-ID: <38BF979F.4CE02BA9@ill.fr>

Hy Kristian,

Well I'm pleased to see that the Monitor_nD appears usefull to you. As a
matter of fact, I made it emulate all the available monitors in McStas 1.2
I also checked it for various combinaisons, but these are so numerous that
bugs may appear latter. If you think about neutron variables that I forgot,
please tell me.
For the official documentation, I don't mind writing it in LaTeX style.
Just give me the format.
My future projects concerning components include the following :
1- I will continue to use an option string, parsed inside the component.
This enables plenty of options with a high verbosity (option really
describes what will be done) and versatility. It reduces the input
parameters, for wich one does not require to know the C identification
name. On the contrary, for future McStas versions evaluating C expressions
for numerical parameters, it won't work. I 'll think about that...
2- I'm planing to also create a kind of generic source, extending the
Flux_adapter, the same manner as Monitor_nD. some work
3- My Optimizer will be modified in order that one may use more that 1
optimisation point (for sequential optimization along instrument). rather
easy
4- In the Monitor_nD I will add the possibility to handle a detection
efficiency.  easy
5- I plan to write a simple amorphous phonon sample using an external
dispersion curve record. This is simple but requires some work

For the common component ressources, I will try to install that this
afternoon.

Thanks.

PS : When will be the next release of McStas (with optional/default params,
string param, sub-directory libs...)

EF.

Kristian Nielsen wrote:

> Hi Emmanuel,
>
> Thanks for the comments. They were as always very useful, and I have
> implemented all of them now (if you find something missing, please let
> me know).
>
> Your generic monitor is very interesting, and I am sure that it will
> prove very useful. I am really hoping that you will write some
> documentation in the same style as all the official components in the
> McStas manual, so that I can include it in the next official
> release. You do not have to use LaTeX, I will convert it for you from
> whatever format you prefer to use.
>
> I have also implemented a method for sharing our component libraries. We
> need to set up a special directory on a web server at each institute
> participating (currently only Ris? and ILL). This directory contains
> ONLY the source code for the components to be shared (ie. my directory
> contains the official components, your directory contains the rest). I
> have written a small shell script,
>
>     http://neutron.risoe.dk/mcstas/support/farhi/builddocs.sh
>
> This script automatically downloads the component source codes from each
> web server into common subdirectories. It then downloads the newest
> mcdoc program from the Ris? server and re-builds all the documentation.
>
> On mica, I have set up a demonstration in the /home/cs/nielsen/mcdoc/
> directory. The command
>
>     ./builddocs.sh
>
> will download all components and build the web pages. Because of the
> firewall, it is necessary to first execute
>
>     setenv http_proxy proxy.ill.fr:8888
>
> What you need to do is to set up a directory on your web server and keep
> it updated with the newest source codes for the components you want to
> share. Then we can both use the builddocs.sh script to create a single
> component page with all components that are automatically kept
> synchronized. What do you think?
>
> Finally, with regard to the mcgui crash on SGI. From yours and Ron's
> emails, I got the impression that this problem was solved with the new
> Perl installation, is this correct?
>
>  - Kristian.
>
> --
> Kristian Nielsen        kristian.nielsen at risoe.dk
> Ris? National Laboratory
> Condensed Matter Physics and Chemistry Department
> Tel. +45 4677 5515   Fax +45 4677 4790
> Encryption PGP key http://neutron.risoe.dk/kn.txt

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue J. Horowitz, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94



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From farhi at ill.fr  Fri Mar  3 14:01:21 2000
From: farhi at ill.fr (Farhi)
Date: Fri, 03 Mar 2000 14:01:21 +0100
Subject: mcdoc ok
Message-ID: <38BFB7A1.788C73F4@ill.fr>

Hy

I've installed the unofficial components in
http://www.ill.fr/tas/mcstas/src/
and updated the web page component index.

Here is my builddocs.sh:

#! /bin/sh

SRCLIST="http://www.ill.fr/tas/mcstas/src/
http://neutron.risoe.dk/mcstas/mcdoc/src/risoe/"
DIRLIST="sources optics samples monitors misc"
MCDOC="http://neutron.risoe.dk/mcstas/mcdoc/src/risoe/mcdoc.pl"

for d in $DIRLIST
do
    rm -Rf $d
    mkdir $d
    for src in $SRCLIST
    do
 (cd $d; wget -nd -L -A comp,cmp,com -r $src/$d/; rm index.html)
    done
done

rm -f mcdoc.pl
wget -nd -L $MCDOC
chmod u+x mcdoc.pl
../mcdoc.pl

I first import the non official, and overload official components. These
latter are then prioritary in case of multiple definitions.
After the process I uploaded the component tree on the Web. All is fine.

The link for the library at Risoe is now
http://neutron.risoe.dk/mcstas/mcdoc/test/.
Should I change it to http://neutron.risoe.dk/mcstas/components/ ?

By the way, yes the perl pb was caused by mixed versions on SGI. All is
ok now.

Bye. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue J. Horowitz, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From kristian.nielsen at risoe.dk  Mon Mar  6 12:58:35 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 6 Mar 2000 12:58:35 +0100
Subject: mcdoc ok
In-Reply-To: <38BFB7A1.788C73F4@ill.fr> (message from Farhi on Fri, 03 Mar
	2000 14:01:21 +0100)
Message-ID: <mailman.106.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Fri, 03 Mar 2000 14:01:21 +0100
> From: Farhi <farhi at ill.fr>

The mcdoc stuff seems to be working great. I have installed a cron job
that automatically updates the Risoe component web pages at 6.10 AM using
both the Risoe and ILL source directories. So whenever you update your
source directory the change should happen on the Risoe pages the next
day. There seems to be a delay from when you make something available
inside ILL to when it appears outside though.

Thanks for the fixes for the builddocs.sh script, by the way. My current
version is at

    http://neutron.risoe.dk/mcstas/mcdoc/src/builddocs.sh

The official name for the Risoe component documentation page is

    http://neutron.risoe.dk/mcstas/mcdoc/components/

I decided not to change the old page
(http://neutron.risoe.dk/mcstas/components/) since that would have
introduced a lot of bad links.

I am happy that the mcgui problem on the SGIs now seems to be solved.

I am not sure when I should release the next version. Maybe once I
finish my current two major projects: multiple scattering in the
Single_crystal component, and extending mcgui to have a user interface
for building instrument definitions (using mcdoc). Shouldn't be too
long.

I think I should not release too often since most users will not want to
install new versions and print out manuals all the time. But I should
also not release too seldom! Two or three times a year seems about
right. In addition I am always happy to release beta versions for
advanced users.

About the Manual format, it is mostly plain LaTex. I have attached the
file for the section on monitors for you to look at.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790
Encryption PGP key http://neutron.risoe.dk/kn.txt

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From kristian.nielsen at risoe.dk  Mon Mar  6 13:38:17 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 6 Mar 2000 13:38:17 +0100
Subject: Automatic generation of component documentation
Message-ID: <mailman.107.1511353198.451.mcstas-users@mailman2.mcstas.org>

Dear Lee,

At the MC workshop at Oak Ridge in January, we briefly discussed the
possibility of automatically generating documentation on components from
comments in the source code itself. The advantage of this approach is
that as the size of the component library grows, the manual maintenance
of the documentation will turn into a nightmare. By using automatic
techniques, documentation can be maintained with a realistic amount of
effort.

Together with Emmanuel Farhi, I have now implemented a first version of
this scheme. The result may be seen on

    http://neutron.risoe.dk/mcstas/mcdoc/components/

Some documentation on the system itself is at

    http://neutron.risoe.dk/mcstas/mcdoc/

In the future, this will also be used to automatically generate
documentation for a graphical user interface to the engine and for the
hardcopy manual.

I thought you might be interested in this. I would be happy to discuss
any questions you may have.

 - Kristian.





From kristian.nielsen at risoe.dk  Tue Mar  7 10:07:32 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 7 Mar 2000 10:07:32 +0100
Subject: IN6 Monochromators
In-Reply-To: <38C3DE33.E3B686C2@ill.fr> (message from Markus Poehlmann on Mon,
	06 Mar 2000 17:34:59 +0100)
Message-ID: <mailman.108.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Mon, 06 Mar 2000 17:34:59 +0100
> From: Markus Poehlmann <poehlman at ill.fr>

> Now I rotated not the arms but the Mosaic_anisotropics themselves and it
> seems that it works. But in the visualisation with mcdisplay a neutron
> passes still one plate after another and is not propagated before having
> passed each of the seven plates in each of the 3 monochromators.
> Is that only a problem of mcdisplay or is the calculation itsself like
> this ? Our results seem to be correct now.

> Would you plaese find attached the file in62.instr and could you please
> have a look on it in respect to the problem described above.

I took a look, and the monochromator setup seems just fine.

The mcdisplay plots can admittedly be confusing sometimes. However, I am
not quite sure what you mean by "a neutron passes still one plate after
another" in mcdisplay? Are you using McStas version 1.2, or is it an
older version?

I have attached three pictures that show a scattering event so that you
can compare with your plots. I have also attached an updated
"Guide.comp" file that allows mcdisplay to show all reflections in the
guide. Also note that the "Bender" component is a little quirky in
mcdisplay because of its non-standard use of geometry.

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790
Encryption PGP key http://neutron.risoe.dk/kn.txt

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/*******************************************************************************
*
* McStas, the neutron ray-tracing package
*         Maintained by Kristian Nielsen and Kim Lefmann,
*         Copyright 1997-2000 Risoe National Laboratory, Roskilde, Denmark
*
* %I
* Written by: KN
* Date: September 2 1998
* Version: $Revision: 1.6 $
* Origin: McStas release
* Modified by: KL, October 6, 1998
*
* Neutron guide.
*
* %D
* Models a rectangular guide tube centered on the Z axis. The entrance lies
* in the X-Y plane.
* For details on the geometry calculation see the description in the McStas
* reference manual.
*
* %P
* INPUT PARAMETERS:
*
* w1:      (m)    Width at the guide entry
* h1:      (m)    Height at the guide entry
* w2:      (m)    Width at the guide exit
* h2:      (m)    Height at the guide exit
* l:       (m)    length of guide
* R0:      (1)    Low-angle reflectivity
* Qc:      (AA-1) Critical scattering vector
* alpha:   (AA)   Slope of reflectivity
* m:       (1)    m-value of material. Zero means completely absorbing.
* W:       (AA-1) Width of supermirror cut-off
*
* %D
* Example values: m=4 Qc=0.02 W=1/300 alpha=6.49 R0=1
*
* %E
*******************************************************************************/

DEFINE COMPONENT Guide
DEFINITION PARAMETERS (w1, h1, w2, h2, l, R0, Qc, alpha, m, W)
SETTING PARAMETERS ()
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)

TRACE
%{
  double t1,t2;                                 /* Intersection times. */
  double av,ah,bv,bh,cv1,cv2,ch1,ch2,d;         /* Intermediate values */
  double vdotn_v1,vdotn_v2,vdotn_h1,vdotn_h2;   /* Dot products. */
  int i;                                        /* Which mirror hit? */
  double q;                                     /* Q [1/AA] of reflection */
  double vlen2,nlen2;                           /* Vector lengths squared */

  /* ToDo: These could be precalculated. */
  double ww = .5*(w2 - w1), hh = .5*(h2 - h1);
  double whalf = .5*w1, hhalf = .5*h1;
  double lwhalf = l*whalf, lhhalf = l*hhalf;

  /* Propagate neutron to guide entrance. */
  PROP_Z0;
  if(x <= -whalf || x >= whalf || y <= -hhalf || y >= hhalf)
    ABSORB;
  for(;;)
  {
    /* Compute the dot products of v and n for the four mirrors. */
    av = l*vx; bv = ww*vz;
    ah = l*vy; bh = hh*vz;
    vdotn_v1 = bv + av;         /* Left vertical */
    vdotn_v2 = bv - av;         /* Right vertical */
    vdotn_h1 = bh + ah;         /* Lower horizontal */
    vdotn_h2 = bh - ah;         /* Upper horizontal */
    /* Compute the dot products of (O - r) and n as c1+c2 and c1-c2 */
    cv1 = -whalf*l - z*ww; cv2 = x*l;
    ch1 = -hhalf*l - z*hh; ch2 = y*l;
    /* Compute intersection times. */
    t1 = (l - z)/vz;
    i = 0;
    if(vdotn_v1 < 0 && (t2 = (cv1 - cv2)/vdotn_v1) < t1)
    {
      t1 = t2;
      i = 1;
    }
    if(vdotn_v2 < 0 && (t2 = (cv1 + cv2)/vdotn_v2) < t1)
    {
      t1 = t2;
      i = 2;
    }
    if(vdotn_h1 < 0 && (t2 = (ch1 - ch2)/vdotn_h1) < t1)
    {
      t1 = t2;
      i = 3;
    }
    if(vdotn_h2 < 0 && (t2 = (ch1 + ch2)/vdotn_h2) < t1)
    {
      t1 = t2;
      i = 4;
    }
    if(i == 0)
      break;                    /* Neutron left guide. */
    PROP_DT(t1);
    switch(i)
    {
      case 1:                   /* Left vertical mirror */
        nlen2 = l*l + ww*ww;
        q = V2Q*(-2)*vdotn_v1/sqrt(nlen2);
        d = 2*vdotn_v1/nlen2;
        vx = vx - d*l;
        vz = vz - d*ww;
        break;
      case 2:                   /* Right vertical mirror */
        nlen2 = l*l + ww*ww;
        q = V2Q*(-2)*vdotn_v2/sqrt(nlen2);
        d = 2*vdotn_v2/nlen2;
        vx = vx + d*l;
        vz = vz - d*ww;
        break;
      case 3:                   /* Lower horizontal mirror */
        nlen2 = l*l + hh*hh;
        q = V2Q*(-2)*vdotn_h1/sqrt(nlen2);
        d = 2*vdotn_h1/nlen2;
        vy = vy - d*l;
        vz = vz - d*hh;
        break;
      case 4:                   /* Upper horizontal mirror */
        nlen2 = l*l + hh*hh;
        q = V2Q*(-2)*vdotn_h2/sqrt(nlen2);
        d = 2*vdotn_h2/nlen2;
        vy = vy + d*l;
        vz = vz - d*hh;
        break;
    }
    /* Now compute reflectivity. */
    if(m == 0)
      ABSORB;
    if(q > Qc)
    {
      double arg = (q-m*Qc)/W;
      if(arg < 10)
        p *= .5*(1-tanh(arg))*(1-alpha*(q-Qc));
      else
        ABSORB;                               /* Cutoff ~ 1E-10 */
    }
    p *= R0;
    SCATTER;
  }
%}

MCDISPLAY
%{
  double x;
  int i;

  magnify("xy");
  multiline(5,
            -w1/2.0, -h1/2.0, 0.0,
             w1/2.0, -h1/2.0, 0.0,
             w1/2.0,  h1/2.0, 0.0,
            -w1/2.0,  h1/2.0, 0.0,
            -w1/2.0, -h1/2.0, 0.0);
  multiline(5,
            -w2/2.0, -h2/2.0, (double)l,
             w2/2.0, -h2/2.0, (double)l,
             w2/2.0,  h2/2.0, (double)l,
            -w2/2.0,  h2/2.0, (double)l,
            -w2/2.0, -h2/2.0, (double)l);
  line(-w1/2.0, -h1/2.0, 0, -w2/2.0, -h2/2.0, (double)l);
  line( w1/2.0, -h1/2.0, 0,  w2/2.0, -h2/2.0, (double)l);
  line( w1/2.0,  h1/2.0, 0,  w2/2.0,  h2/2.0, (double)l);
  line(-w1/2.0,  h1/2.0, 0, -w2/2.0,  h2/2.0, (double)l);
%}

END

From poehlman at ill.fr  Mon Mar  6 17:34:59 2000
From: poehlman at ill.fr (Markus Poehlmann)
Date: Mon, 06 Mar 2000 17:34:59 +0100
Subject: IN6 Monochromators
Message-ID: <38C3DE33.E3B686C2@ill.fr>

Dear Kristian,

thank you very much for your detailled help. I think, I succeeded now
with the simplest method of rotating 7 Mosaic_anistropic components
three times. We tried the same method some weeks ago by defining a
certain Arm() for each of the 7 monochromators. But that did not work,
as Helmut wrote to you. The result was that McStas was trying to force
the neutrons from one plate to another.
Now I rotated not the arms but the Mosaic_anisotropics themselves and it
seems that it works. But in the visualisation with mcdisplay a neutron
passes still one plate after another and is not propagated before having
passed each of the seven plates in each of the 3 monochromators.
Is that only a problem of mcdisplay or is the calculation itsself like
this ? Our results seem to be correct now.
Would you plaese find attached the file in62.instr and could you please
have a look on it in respect to the problem described above.
Thanks a lot again

Markus Poehlmann
-------------- next part --------------
%include "mono2.comp"
/*%include "monoscatt.comp"
%include "monoscatt1.comp"%*/

DEFINE INSTRUMENT IN6 (lamda_i,dlamda_i)  
/* A template IN6 simulation for McStas. M. Poehlmann <poehlman at ill.fr> feb 00 
 * input parameters : 
 *     lamda_i : incident n-wavevector [Angs-1] 
 *     dlamda_i: spread of incident n-wavevector [Angs-1]*/

DECLARE 

%{
/* all variables defined here can be used, and modified, in the whole instrument */ 
/* variables used in instrument definition and for user computations */ 


double DM = 3.355;     /*   mono d-spacing (Angs)  */
double DA = 3.355;     /*   ana d-spacing   */

/* Bragg angles of the 3 monochromators */
double A1;
double A1half;
double A1strich;
double A2;
double A2half;
double A2strich;
double A3;
double A3half;
double A3,A4,A5,A6; /* geometrical angles (deg) */ 

double Ki;          /*incident wave vector corresponding to lamda_i */
double dKi;         /*spread of incident wave vector <--> dlamda_i  */

double mono_q;      /* Q vector for bragg scattering with monochromator */ 
double ana_q;       /* Q vector for bragg scattering with analyzer */ 
double Ei = 0;      /* incident n-energy */ 
double dEi = 0;     /* energy spread of source neutrons*/
double Ef = 0;      /* out-going n-energy */ 
double Kf = 0;      /* out-going n-wavevector */ 
double Q = 0;

double d1 = 3.0;    /*distance guide 2 <--> monochromator*/
double l2 = 2.1;    /*distance monochromator 2 <--> sample*/
double li = 0.03;   /*distance between 2 monochromators*/
double position_m1; /*position of monochromator 1 relative end of guide 2*/
double position_m2; /*                          2                        */
double position_m3; /*                          3                        */

char flag_scattered;



/* defintion of variables for calculation of positions of 7 monochromators*/
double  r = 3.0;
int i;
double phi[7];
double z[7];
double y[7];
double x[7];
double PHI1, PHI2, PHI3, PHI4, PHI5, PHI6, PHI7;
double x_1, x_2, x_3, x_4, x_5, x_6, x_7;
double y_1, y_2, y_3, y_4, y_5, y_6, y_7;
double z_1, z_2, z_3, z_4, z_5, z_6, z_7;

%} 
/* end of DECLARE */ 

INITIALIZE
 
%{ 

/* variables defined here are local (only in INIT section) */ 
/* can be computed / displayed (see below) */ 
double Vi = 0;      /* incident n-velocity (m/s) */ 
double dVi;         /* incident spread of n-velocity */
double Vf = 0;      /* out-going n-velocity */ 
int    SM,SS,SA;    /* rotation sign */ 
double arg = 0;     /* tempo var */ 
int    ORDER = 1; 
/* dealing with ORDERth Bragg one-neutron diffraction on mono/ana */ 

/* SM : scattering at mono to the right (-1)/left(+1) */ 
/* SS : scattering at sample to the right (-1)/left(+1) */ 
/* SA : scattering at analyser to the right (-1)/left(+1) */ 
SM = -1; SS = -1; SA = 1; 

mono_q = 2*PI*ORDER/DM;  /* Q mono in Angs-1 */ 

position_m1 = d1-li;
position_m2 = d1;
position_m3 = d1+li;


Ki = 2*PI/lamda_i;
dKi = 2*PI*dlamda_i/(lamda_i*lamda_i);
Vi = K2V*fabs(Ki); 
Ei = VS2E*Vi*Vi;
dVi = K2V*dKi;
dEi = 2*VS2E*Vi*dVi;
printf("Ki=%lf\tdKi=%lf\tEi=%lf\tdEi=%lf\n",Ki,dKi,Ei,dEi);

if (dEi>Ei)
{
  printf("The energy spread dEi is greater than the energy Ei.\n");
  printf("Please insert a smaller dlamda_i.\n");
  exit(-1);
}
  
/*calculate theta angles for 3 monochromators*/

A2 = asin(mono_q/2/Ki)*2;
A2 *= SM;   /* A : mono theta (crystal) */

A1 = atan(l2*sin(A2)/(li+l2*cos(A2)))*RAD2DEG;
A1 *= -SM;
A1half = A1/2.0;

A3 = atan(l2*sin(A2)/(l2*cos(A2)-li))*RAD2DEG;
A3 *= -SM;
A3half = A3/2.0;

A2 *=RAD2DEG;
A2strich=-A2;  
A2half = A2/2.0; 

printf("A1=%lf\tA2=%lf\tA3=%lf\n",A1,A2,A3);

/* Analyzer characteristics (A5,A6 from Kf, DA) */ 
Vf = SE2V*sqrt(Ei);     /* final energy from energy transfert */ 
Kf = V2K*Vf; 
if (DA <= 0.1) 
{ 
  printf("TAS: Ana DA = %f Angs, too small\n", DM); 
  exit(-1); 
} 
ana_q = 2*PI*ORDER/DA;  /* Q ana in Angs-1 */ 
if ((Kf == 0) || (fabs(mono_q/2/Kf) > 1)) 
{ 
  printf("TAS: Can not reach this out-going wavevector\n"); 
  printf("     with such an analyzer (A6)\n"); 
  printf("Mono DA = %f Angs, requested Kf = %f Angs-1\n", DA, Kf); 
  exit(-1); 
} 
A6 = asin(ana_q/2/Kf)*RAD2DEG*2; 
A6 *= SA;   /* A5 : analyser theta (crystal) */ 
A5  = A6/2; /* A6 : analyser 2 theta (arm to detector) */ 

/* Sample characteristics */
arg = (Ki*Ki + Kf*Kf - Q*Q)/2/fabs(Ki*Kf); 
/*if (fabs(arg) > 1) 
{ 
  printf("TAS: Can not close wavevector triangle (A4)\n"); 
  printf("Incident Ki = %f Angs-1, Exchange Q=%f Angs-1, Final Kf = %f Angs-1\n",Ki,Q,Kf); 
  exit(-1); 
} */
A4 = acos(arg)*RAD2DEG; 
A4 *= SS;   /* A4 : sample 2 theta (arm to analyser) */ 

/* computing of A3 requires sample reciprocal axes characteristics */ 
A3  = A4/2; /* A3 : sample theta 

printf("IN14 at ILL 3-axis spectrometer\n"); 
printf("Angles (deg) A1 = %f ; A4 = %f ; A6 = %f\n",A2,A4,A6);*/ 

for(i=0;i<=6;i++)
  {
    phi[i]=(-0.087+0.029*i)/r;
    x[i]=-r*(1-cos(phi[i])); 
    y[i]=r*sin(phi[i]);
    z[i]=-r*(1-cos(phi[i]));
    phi[i]*=RAD2DEG;
  }
  PHI1=phi[0]; PHI2=phi[1]; PHI3=phi[2]; 
  PHI4=phi[3]; PHI5=phi[4]; PHI6=phi[5]; PHI7=phi[6];
  x_1=x[0]; x_2=x[1]; x_3=x[2]; x_4=x[3]; x_5=x[4]; x_6=x[5]; x_7=x[6];
  y_1=y[0]; y_2=y[1]; y_3=y[2]; y_4=y[3]; y_5=y[4]; y_6=y[5]; y_7=y[6];
  z_1=z[0]; z_2=z[1]; z_3=z[2]; z_4=z[3]; z_5=z[4]; z_6=z[5]; z_7=z[6];
%}


TRACE
 
/* Source description */ 
COMPONENT source = Source_flux( /* a flat constant source */ 
 radius = 0.20, 
 dist =2.27, 
 xw = 0.038, yh = 0.2, 
 E0 = Ei, 
 dE = dEi, 
 flux=1e13) 
AT (0,0,0) ABSOLUTE

/*COMPONENT PSD_source = PSD_monitor( 
  xmin = -0.1, xmax = 0.1, 
  ymin = -0.1, ymax = 0.1, 
  nx = 100, ny = 100, 
  filename="source.psd") 
AT (0, 0, 0) RELATIVE source

COMPONENT E_source= E_monitor(
  xmin=-.1, xmax=.1,
  ymin=-.1, ymax=.1,
  Emin=0, Emax=10,
  nchan=100,
  filename="E_source.emo")
AT (0,0,0.000001) RELATIVE source


COMPONENT PSD_3_12 = PSD_monitor( 
  xmin = -0.1, xmax = 0.1, 
  ymin = -0.1, ymax = 0.1, 
  nx = 100, ny = 100, 
  filename="3_12.psd") 
AT (0, 0, 3.12) RELATIVE source

COMPONENT E_3_12 = E_monitor(
  xmin=-.1, xmax=.1,
  ymin=-.1, ymax=.1,
  Emin=0, Emax=10,
  nchan=100,
  filename="E_vor_guide_1.emo")
AT (0,0,0.00001) RELATIVE PSD_3_12*/

COMPONENT guide_1 = Guide(
  w1=0.038, h1=0.2,
  w2=0.032, h2=0.2,
  l=3.68,
  R0=1,
  Qc=0.02176,
  alpha=2.33,
  m=1.2,
  W=2e-3)
AT (0,0,3.12001) RELATIVE source 

COMPONENT PSD_guide_1 = PSD_monitor( 
  xmin = -0.1, xmax = 0.1, 
  ymin = -0.1, ymax = 0.1, 
  nx = 100, ny = 100, 
  filename="guide_1.psd") 
AT (0, 0, 6.8) RELATIVE source

COMPONENT E_guide_1 = E_monitor(
  xmin=-.1, xmax=.1,
  ymin=-.1, ymax=.1,
  Emin=0, Emax=10,
  nchan=100,
  filename="E_guide_1.emo")
AT (0,0,0) RELATIVE PSD_guide_1

COMPONENT bender1 = Bender(
  w=0.03,
  h=0.2,
  r=2700.0,
  d=0,
  Win=0.0101851,
  k=1,
  R0a=1, Qca=0.02176, alphaa=2.33, ma=1.2, Wa=2e-3, 
  R0i=1, Qci=0.02176, alphai=2.33, mi=1.2, Wi=2e-3,
  R0s=1, Qcs=0.02176, alphas=2.33, ms=1.2, Ws=2e-3)
AT (0,0,3.68) RELATIVE guide_1

COMPONENT PSD_bender1 = PSD_monitor( 
  xmin = -0.1, xmax = 0.1, 
  ymin = -0.1, ymax = 0.1, 
  nx = 100, ny = 100, 
  filename="bender1.psd") 
AT (0, 0, 27.5) RELATIVE bender1

COMPONENT E_bender1 = E_monitor(
  xmin=-.1, xmax=.1,
  ymin=-.1, ymax=.1,
  Emin=0, Emax=10,
  nchan=100,
  filename="E_bender1.emo")
AT (0,0,0) RELATIVE PSD_bender1

COMPONENT guide_2 = Guide(
  w1=0.032, h1=0.2,
  w2=0.032, h2=0.2,
  l=27,
  R0=1,
  Qc=0.02176,
  alpha=2.33,
  m=1.2,
  W=2e-3)
AT (0,0,27.5) RELATIVE bender1 

COMPONENT PSD_guide_2 = PSD_monitor( 
  xmin = -0.1, xmax = 0.1, 
  ymin = -0.1, ymax = 0.1, 
  nx = 100, ny = 100, 
  filename="guide_2.psd") 
AT (0, 0, 27) RELATIVE guide_2

COMPONENT E_guide_2 = E_monitor(
  xmin=-.1, xmax=.1,
  ymin=-.1, ymax=.1,
  Emin=0, Emax=10,
  nchan=100,
  filename="E_guide_2.emo")
AT (0,0,0) RELATIVE PSD_guide_2

COMPONENT a1 = Arm() AT (0,0,27) RELATIVE guide_2

COMPONENT arm_M1 = Arm() AT (0,0,position_m1) RELATIVE a1 
                           ROTATED (0,A1half,0) RELATIVE a1 

COMPONENT m11 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_1,y_1,0) RELATIVE arm_M1 ROTATED (0,0,PHI1) RELATIVE arm_M1

COMPONENT m12 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_2,y_2,0) RELATIVE arm_M1 ROTATED (0,0,PHI2) RELATIVE arm_M1

COMPONENT m13 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_3,y_3,0) RELATIVE arm_M1 ROTATED (0,0,PHI3) RELATIVE arm_M1

COMPONENT m14 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_4,y_4,0) RELATIVE arm_M1 ROTATED (0,0,PHI4) RELATIVE arm_M1 

COMPONENT m15 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_5,y_5,0) RELATIVE arm_M1 ROTATED (0,0,PHI5) RELATIVE arm_M1

COMPONENT m16 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_6,y_6,0) RELATIVE arm_M1 ROTATED (0,0,PHI6) RELATIVE arm_M1

COMPONENT m17 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_7,y_7,0) RELATIVE arm_M1 ROTATED (0,0,PHI7) RELATIVE arm_M1


COMPONENT arm_M2 = Arm() AT (0,0,position_m2) RELATIVE a1 
                           ROTATED (0,A2half,0) RELATIVE a1 

COMPONENT m21 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_1,y_1,0) RELATIVE arm_M2 ROTATED (0,0,PHI1) RELATIVE arm_M2

COMPONENT m22 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_2,y_2,0) RELATIVE arm_M2 ROTATED (0,0,PHI2) RELATIVE arm_M2

COMPONENT m23 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_3,y_3,0) RELATIVE arm_M2 ROTATED (0,0,PHI3) RELATIVE arm_M2

COMPONENT m24 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_4,y_4,0) RELATIVE arm_M2 ROTATED (0,0,PHI4) RELATIVE arm_M2 

COMPONENT m25 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_5,y_5,0) RELATIVE arm_M2 ROTATED (0,0,PHI5) RELATIVE arm_M2

COMPONENT m26 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_6,y_6,0) RELATIVE arm_M2 ROTATED (0,0,PHI6) RELATIVE arm_M2

COMPONENT m27 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_7,y_7,0) RELATIVE arm_M2 ROTATED (0,0,PHI7) RELATIVE arm_M2

COMPONENT arm_M3 = Arm() AT (0,0,position_m3) RELATIVE a1 
                           ROTATED (0,A3half,0) RELATIVE a1 

COMPONENT m31 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_1,y_1,0) RELATIVE arm_M3 ROTATED (0,0,PHI1) RELATIVE arm_M3

COMPONENT m32 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_2,y_2,0) RELATIVE arm_M3 ROTATED (0,0,PHI2) RELATIVE arm_M3

COMPONENT m33 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_3,y_3,0) RELATIVE arm_M3 ROTATED (0,0,PHI3) RELATIVE arm_M3

COMPONENT m34 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_4,y_4,0) RELATIVE arm_M3 ROTATED (0,0,PHI4) RELATIVE arm_M3 

COMPONENT m35 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_5,y_5,0) RELATIVE arm_M3 ROTATED (0,0,PHI5) RELATIVE arm_M3

COMPONENT m36 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_6,y_6,0) RELATIVE arm_M3 ROTATED (0,0,PHI6) RELATIVE arm_M3

COMPONENT m37 = Mosaic_anisotropic(
  zmin=-0.015, zmax=0.015, ymin=-0.014, ymax=0.014,
  mosaich=50, mosaicv=50,
  r0=0.95,
  Q=mono_q) 
AT (x_7,y_7,0) RELATIVE arm_M3 ROTATED (0,0,PHI7) RELATIVE arm_M3


COMPONENT 4PI_mono = PSD_monitor_4PI(
  radius=2.1,
  nx=100, ny=100,
  filename="4PI_mono.psd")
AT (0,0,d1) relative a1

COMPONENT focus_sample = Arm()
AT (0,0,d1) RELATIVE a1 ROTATED (0,A2,0) RELATIVE a1

COMPONENT anti_focus_sample = Arm()
AT (0,0,d1) RELATIVE a1 ROTATED (0,A2strich,0) RELATIVE a1

COMPONENT PSD_mono = PSD_monitor( 
  xmin = -0.1, xmax = 0.1, 
  ymin = -0.1, ymax = 0.1, 
  nx = 100, ny = 100, 
  filename="mono.psd") 
AT (0, 0, l2) RELATIVE focus_sample 

/*COMPONENT anti_PSD_mono = PSD_monitor( 
  xmin = -0.1, xmax = 0.1, 
  ymin = -0.1, ymax = 0.1, 
  nx = 100, ny = 100, 
  filename="anti_mono.psd") 
AT (0, 0, l2) RELATIVE anti_focus_sample*/ 

/*COMPONENT dreh_PSD_mono = PSD_monitor( 
  xmin = -30, xmax = 30, 
  ymin = -30, ymax = 30, 
  nx = 100, ny = 100, 
  filename="dreh_mono.psd") 
AT (0, 0, 3) RELATIVE arm_M1_2 */


COMPONENT E_mono = E_monitor(
  xmin=-0.1, xmax=0.1,
  ymin=-0.1, ymax=0.1,
  Emin=3, Emax=4.5,
  nchan=100,
  filename="E_mono.emo")
AT (0,0,0) RELATIVE PSD_mono

COMPONENT PSD_mono_test = PSD_monitor( 
  xmin = -1, xmax = 1, 
  ymin = -1, ymax = 1, 
  nx = 100, ny = 100, 
  filename="mono_test.psd") 
AT (0, 0, 3.3) RELATIVE a1   

/*COMPONENT mono_1 = Monochromator(
  zmin=-*/


END





























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From hansen at ill.fr  Mon Mar 13 11:23:43 2000
From: hansen at ill.fr (Thomas C Hansen)
Date: Mon, 13 Mar 2000 11:23:43 +0100
Subject: mcdoc - default values for input parameters
Message-ID: <38CCBF41.A729DE59@ill.fr>

Dear Kristian and Emmanuel,

The tables in the html files coming out from mcdoc contain a column for default
values of input parameters. I haven't found any component alrady using this
possibility, so what's the foreseen syntax to fill in that column as well?

Thanks for reply!

Thomas









From kristian.nielsen at risoe.dk  Mon Mar 13 11:17:38 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 13 Mar 2000 11:17:38 +0100
Subject: mcdoc - default values for input parameters
In-Reply-To: <38CCBF41.A729DE59@ill.fr> (message from Thomas C Hansen on Mon,
	13 Mar 2000 11:23:43 +0100)
Message-ID: <mailman.109.1511353198.451.mcstas-users@mailman2.mcstas.org>

> Date: Mon, 13 Mar 2000 11:23:43 +0100
> From: Thomas C Hansen <hansen at ill.fr>

> Dear Kristian and Emmanuel,
> 
> The tables in the html files coming out from mcdoc contain a column for default
> values of input parameters. I haven't found any component alrady using this
> possibility, so what's the foreseen syntax to fill in that column as well?

For example,

  DEFINE COMPONENT GUIDE
  SETTING PARAMETERS(R0 = 1, ...)

This would make the R0 parameter optional, with a default value of
1. This is already implemented in my current development version. I
guess a similar syntax will be implemented for instrument input
parameters.

 - Kristian.





From farhi at ill.fr  Wed Mar  8 14:11:32 2000
From: farhi at ill.fr (Farhi)
Date: Wed, 08 Mar 2000 14:11:32 +0100
Subject: About spin ?
Message-ID: <38C65184.E3C7A706@ill.fr>

Hy Kristian

I'm now writing the documentation for components Source_Optimizer,
Monitor_Optimizer and Monitor_nD. Hope it will be clear and usefull.
I was wondering what you think about neutron spin. I mean the fact that
you have s1 and s2 [ STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p) ] in
all components,
but you do not have (sx, sy, sz) except if you really ask for it [
POLARISATION PARAMETERS (sx,sy,sz) ]. In this latter case, one usually
get huge amounts of warning from other components. This is very starnge
as s1 and s2 should contain the same information as sx sy sz, but in a
different way.

What about writing a MACRO that would compute sx, sy sz from s1 and s2,
according to the component orientation, and possibly neutron direction,
and an other one that would do the reverse operation ?

This would make all component beeing able to handle polarisation, and
would thus avoid warnings.

Also, I just point out that writing a component that does or does not
handle polarisation with POLARISATION PARAMETERS symbol makes two way of
programming : in one hand you will use s1 s2, in the other, sx sy sz....

Cheers. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue J. Horowitz, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From farhi at ill.fr  Thu Mar  9 18:17:58 2000
From: farhi at ill.fr (Farhi)
Date: Thu, 09 Mar 2000 18:17:58 +0100
Subject: Doc for components
Message-ID: <38C7DCC6.58D912AC@ill.fr>

Hy Kristian,

Here is a documentation in LaTeX format for the Source_optimizer and
monitor_nD components.
Feel free of any remarks !! (I just finished it, and I'm tired...)

Cheers. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue J. Horowitz, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From kristian.nielsen at risoe.dk  Wed Mar 15 13:16:28 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 15 Mar 2000 13:16:28 +0100
Subject: About spin ?
In-Reply-To: <38C65184.E3C7A706@ill.fr> (message from Farhi on Wed, 08 Mar
	2000 14:11:32 +0100)
Message-ID: <mailman.110.1511353199.451.mcstas-users@mailman2.mcstas.org>

Hi Emmanuel,

Thanks a lot for the Latex manual entries. I will look closer at them
and include them the next time I revise the manual.

I just finished a new version of mcgui which integrates the mcdoc stuff
so that components can be used in a "user-friendly" graphics dialog
(also works for the users own components in the current
directory). While I am not completely satisfied with it yet, I think it
is promising and will be quite useful. I have put an "alpha" release up
for you on the web page at

    http://neutron.risoe.dk/mcstas/support/farhi/mcstas-1.23A.tar.gz

in case you want to try it out and have some comments. It also has the
new string instrument parameters and optional component parameters, but
be careful about using them since your code will then not work in McStas
1.2! To see the new mcgui stuff you need to open the integrated editor
window and use the new "Insert" menu.

About the neutron spin: When I visited ILL last year, I had some
discussions with Trefor, and we agreed that the polarisation needed to
have three components (though I can no longer remember why). However,
that is not the reason for having a separate "POLARISATION PARAMETERS"
statement instead of using the STATE PARAMETERS. Rather, the reason is
to provide a way for components to advertise that they know how to
propagate the neutron spin through the guide field properly. Just
mentioning the spin in the STATE PARAMETERS without doing anything about
them does not properly handle polarisation in all cases! Therefore the
warning is telling the user that the component completely ignores
polarisation, which was probably not intended. If it is useful, we can
allow two-component polarisation, but that will also use the
POLARISATION PARAMETER syntax, not STATE PARAMETER. The s1 and s2 STATE
PARAMETERS will soon be removed (but still ignored if present for
backward compatibility).

I am now planning to release the next version of McStas at the SCANS
meeting at the ILL on May 18.

 - Kristian.

--
Kristian Nielsen        kristian.nielsen at risoe.dk
Ris? National Laboratory
Condensed Matter Physics and Chemistry Department
Tel. +45 4677 5515   Fax +45 4677 4790
Encryption PGP key http://neutron.risoe.dk/kn.txt





From farhi at ill.fr  Fri Mar 10 15:30:53 2000
From: farhi at ill.fr (Farhi)
Date: Fri, 10 Mar 2000 15:30:53 +0100
Subject: Output parameters
Message-ID: <38C9071D.D7EC7DF7@ill.fr>

Hy

I have adopted a solution for the numerous output parameters I had in my
components : I put all of them into structures. Thus there is only one
symbol than contains all the data. Then, the Monitor_Optimizer uses the
same principle as your Adapt_check for getting the information :
MC_GETPAR with the optimizer name from the instrument definition. This
adds an input parameter to Monitor_Optimizer. I updated this fact in the
doc attached.

Cheers.
EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue J. Horowitz, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From kristian.nielsen at risoe.dk  Tue Mar 28 12:06:10 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 28 Mar 2000 12:06:10 +0200
Subject: Position and targeting
In-Reply-To: <38E06590.7328958C@ill.fr> (message from Farhi on Tue, 28 Mar
	2000 09:56:00 +0200)
Message-ID: <mailman.111.1511353199.451.mcstas-users@mailman2.mcstas.org>

> Date: Tue, 28 Mar 2000 09:56:00 +0200
> From: Farhi <farhi at ill.fr>

> I'm designing a general source for McStas, with option string such as
> for the Monitor_nD (enabling many cross-options and extended
> customization). For this, a possible option for source (and usefull !)
> is to target to a specified component. For this, I need to get the
> distance from the source to the next component. This is stored into the
> 'mcposa*' structures, but these are defined AFTER the initialization of
> all components. In order to be able to use these informations during
> init of components, would it be possible to move the /* Computation of
> coordinate transformations. */ at the begining of the mcinit function ?
> Then with a
> #define MC_GETPOS(comp) (mcrota ## comp )
> it would be possible to access all component positions during init of
> components...

Yes, I have intended to implement something like this for a long
time. It is clearly needed for components to be able to ask for the
position of other components like you suggest. There was some
complitation (can't remember what just now), but it should clearly be
possible. I will try go get it done for the next release in May (or
sooner, if it turns out to be very simple).

I am also thinking that it would be useful to support the "option style"
that you have used so successfully in a better way in the McStas core?
Either through extended syntax, or with some library calls for
components.

Another thing: Did you notice that the McDoc documentation on the Ris? Web
pages for your Flux_adapter is messed up? The reason seems to be that
the automatic script downloads an old version of the file. In fact, I
just tried to download the Flux_adapter.comp source from

    http://www.ill.fr/tas/mcstas/src/sources/Flux_adapter.comp

and that is indeed an old version without McDoc tags. Any idea what
might be wrong?

 - Kristian.





From u840163 at oz.nthu.edu.tw  Wed Mar 29 04:56:17 2000
From: u840163 at oz.nthu.edu.tw (=?big5?B?sWmyS6l8?=)
Date: Wed, 29 Mar 2000 10:56:17 +0800
Subject: Thanks  for  your  program , and I  need  a  help
Message-ID: <38E170D0.31B29873@oz.nthu.edu.tw>

Dear  Dr.  Kristian  and  Dr.  Nielsen

How do you do!

Nice to write to you!

I  am  a  student  , and  now I am trying to simulate a instrument  for
SANS (Small angle

neutron scattering ) of  nuclear  reactor.

I  have downloaded  your  simulation  program. I  try  to  make  up  a
system  for  your

simulation  program. And  the  sourround   seemed  to  be  accepted  by
your  program .

I  have  tried  the  examples . It  compiles  and  calculates
successfully .

But  now,  I  contact  some  problems , like  the  form  after
calculated  ,what  it  means ,

and  how  should  I  tran  the  data  into  a  graph .Or  the  other
forms  that  I  can  get

the  informations  more  clearly . And  I  want  to  know  the
flowchart  to  use  your

program  after  it  have  installed  on  our  workstation more  detail .

Otherwise , can  you  give  me  the  informatins , insturments , and
programs  about

SANS ( Small  angle  neutron  scattering ) .

I  need  your  help , can  you  do  me  a  favor .

Thanks  a  lot .


                                                      Tain-Shang  Chang

                                                       E-mail :
u840163 at oz.nthu.edu.tw

                                                      National  Tsing
Hua  University ,  R . O . C
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From kristian.nielsen at risoe.dk  Wed Mar 29 08:57:26 2000
From: kristian.nielsen at risoe.dk (Kristian Nielsen)
Date: 29 Mar 2000 08:57:26 +0200
Subject: Thanks  for  your  program , and I  need  a  help
In-Reply-To: <38E170D0.31B29873@oz.nthu.edu.tw> (message from	=?big5?B?sWmyS6l8?= on Wed, 29 Mar 2000 10:56:17 +0800)
Message-ID: <mailman.112.1511353199.451.mcstas-users@mailman2.mcstas.org>

Dear Tain-Shang Chang,

It sounds like you have successfully installed McStas on your
computers, which is good. You do not say which version of McStas you are
using (the command "mcstas --version" will tell you). I would recommend
that you use the latest release, version 1.2. You should also make sure
that you have the latest manual (I can send a hardcopy if you have
trouble downloading and printing).

If McStas has been fully installed, you can use the "mcplot" and "mcgui"
programs to plot the results. See the manual sections 2.6.1 and
2.6.5. Otherwise you need some other program (gnuplot, matlab, origin,
excel, ...). The data files are in ascii formats that most programs will
read, see the manual section 2.7.

For a simple introduction to the use of the porgram you should read the
McStas tutorial. This may be downloaded from

    http://neutron.risoe.dk/mcstas/tutorial/tutorial.pdf

I am not sure if anyone have attempted detailed SANS simulations using
McStas, but there should be no fundamental problems.

 - Kristian.





From farhi at ill.fr  Thu Mar 16 12:42:07 2000
From: farhi at ill.fr (Farhi)
Date: Thu, 16 Mar 2000 12:42:07 +0100
Subject: McStas 1.23 checked
Message-ID: <38D0C88F.F471839@ill.fr>

Hello Kristian,

I've just tested this new version. It's nice as usual !
Seems ok as long as components have the good format (and this forces
authors to write components with good format).
The 'Inser/Component...' presents abstracts of components, and that is
good.
I guess the 'Other' can retreive local components too. A problem exists
when a componnet exists in the root lib, and in sbdirectories... This
will be cleared when all components will be sorted in subdirectories. A
installed a local comp near instrument file, but mcgui could not see it
(user components).

Cheers. EF

I go on testing...

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue J. Horowitz, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From farhi at ill.fr  Thu Mar 16 13:54:46 2000
From: farhi at ill.fr (Farhi)
Date: Thu, 16 Mar 2000 13:54:46 +0100
Subject: component location
Message-ID: <38D0D996.C6F8E5A8@ill.fr>

Hy again,

in the McGui Editor/Insert menu/Component -> Select component definition
dialog, it would be quite usefull to also display the location of the
component (full path).
This would be easier to sort what components are used, and where the
components are accessed (various LIB pathes searched by McStas):
MCSTAS_LIB/
MCSTAS_LIB/subdirectories
local path (where the instrument is)

You can also optionally add a Help menu item calling Web pages at Risoe.

I've added the components made by Thomas Hansen in ILL src directory. It
should appear tomorrow at Risoe.
The user components are scaned by McGui at startup, thus I can now see
the component that I added near the instrument. OK.

Cheers. EF.

--
Emmanuel FARHI, http://www.ill.fr/tas/people/Farhi.html     \|/ ____ \|/
TAS-Group, Institut Laue-Langevin (ILL) Grenoble            ~@-/ oO \-@~
Avenue J. Horowitz, BP 156, 38042 Grenoble Cedex 9,France   /_( \__/ )_\
Work :Tel (33/0) 4 76 20 71 83. Fax (33/0) 4 76 48 39 06       \__U_/
La Grande Arche, Chateau d'Uriage, 38410 Saint Martin d'Uriage 04 76 59 73 94


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From hansen at ill.fr  Mon Mar  6 10:54:48 2000
From: hansen at ill.fr (Thomas C Hansen)
Date: Mon, 06 Mar 2000 10:54:48 +0100
Subject: commandline arguments in mcstas
Message-ID: <38C38066.4435370B@ill.fr>

Dear Kristian,

In a future version of McStas, could you imagine some additional funcitonality
in the commandline arguments of mcstas simulations? E.g. for a huge number of
parameters, in the actual version the commandline becomes too long, so the only
way is to give all parameters manually, or by a commandline like
'./mysimulation.out -n 1e6 < input.arguments'. That workaround is fine, as long
as I do not want to use gscan which won't work by no means, if there are too
many parameters. I could imagine a commandline like './mysimulation.out -n 1e6
-p input.arguments Lmin=1.2 Lmax=1.4', which means, all input parameters are
taken from a file input.arguments, except the parameters Lmin and Lmax, which
are overwritten by the values given in the commandline. This procedure would
permit the use of a slightly modified version of gscan (taking account of the
option '-p' or '--param' of the mcstas generated simulation). The file
input.arguments might contain as many 'param=value', separated by linefeed,
blank or comma in any order. If any 'param=value' is missing in the file
input.arguments, as well as in the commandline itself, the up to now used
convention may be used, which is asking interactively the user for some input.
(That's in fact another, new, suggestion, as in the actual version the
simulation stops if some parameters are given, others not. Why not asking
interactively these missing parameters instead?)

These are just suggestions, in order to ripe some new ideas, don't take it as a
strong demand right now!

Best Regards,

Thomas


--
Dr. Thomas C HANSEN, Instrument Scientist D20, Diffraction Group
Institut Max von Laue-Paul Langevin, BP 156, 38042 Grenoble C?dex 9, France
ILL4-1st floor room 100, Phone +33(0)476207044, Fax +33(0)476207648
mailto:hansen at ill.fr, http://www.ill.fr/YellowBook/D20
Private: 13, all?e des ?tangs, 38240 Meylan, France, +33(0)476180553







From hansen at ill.fr  Fri Mar 10 08:22:30 2000
From: hansen at ill.fr (Thomas C Hansen)
Date: Fri, 10 Mar 2000 08:22:30 +0100
Subject: McDoc also for instruments?
Message-ID: <38C8A2B5.F8DF2664@ill.fr>

Good morning, Kristian and Emmanuel!

Just a short suggestion for McDoc (I suppose it is foreseen for the next McStas
release to search components also recursively in the subdirectories, e.g.
../sources/, ./monitors/, etc., of a given or the default directory if not found
there): A similar perl procedure could be applied in the same time as well to
instrument descriptions (*.instr, etc.), to be placed in another subdirectory
'instruments' or so. Probably you've already thought of this ...

Have a nice day - and thanks for McDoc!

Thomas






From hansen at ill.fr  Mon Mar 13 15:14:40 2000
From: hansen at ill.fr (Thomas C Hansen)
Date: Mon, 13 Mar 2000 15:14:40 +0100
Subject: mcdoc - default values for input parameters
References: <01JMZDJ3ELEC8X2R4E@risoe.dk>
Message-ID: <38CCF7CE.94307BFA@ill.fr>

Dear Kristian,

I see your approach, looks good! By the way, I wrote a perl script (attached), which
handles huge command lines, as I suggested a couple of days ago. To use it, you put
all my files in a directory and type, e.g.,

ln -s mcsim.pl mcsim; chmod a+x mcsim
mcsim d20 par=ge113.par Sample_file=0

This will call 'mcrun d20', take default parameters from 'd20.par', overwrite them
with parameters eventually found in 'ge113.par', and overwrite in the end the
parameter 'Sample_file'. If any needed parameter as found in 'd20.instr' is missing,
the script will ask for it and append a corresponding entry in 'd20.par'. All these
parameters are not simply given in a command line, as this won't work for command
lines above a certain limited length, but only the values are written in the right
order in a temporary file 'd20.stdin'. Then a shell script containing 'mcrun d20 <
d20.stdin > d20.stdout' is executed. In order to suppress all messages asking for
all these parameters, the output is deviated to 'd20.stdout' and the script is
printing in the end only lines not containing these questions to the screen.
Unfortunately I haven't found yet a possibility to filter that standard output in
real time - that would be preferable. With this perl script also gscan will work,
using e.g. following command line:

gscan 10 1e5 mcsim d20.scan instr=d20 par=ge113.par Source_N_E=1,10

That's just a suggestion, it works fine for me, but maybe some future testing and
standardization has to be done to make it a secure tool for everybody handling long
lists of parameters. It will be easy to adapt the script to default values as you
suggested, just by an additional string analysis of the 'DEFINE INSTRUMENT'
following lines. In that case a default parameter file ('d20.par' in the example)
may become redundant.

Best Regards,

Thomas


Kristian Nielsen wrote:

> > Date: Mon, 13 Mar 2000 11:23:43 +0100
> > From: Thomas C Hansen <hansen at ill.fr>
>
> > Dear Kristian and Emmanuel,
> >
> > The tables in the html files coming out from mcdoc contain a column for default
> > values of input parameters. I haven't found any component alrady using this
> > possibility, so what's the foreseen syntax to fill in that column as well?
>
> For example,
>
>   DEFINE COMPONENT GUIDE
>   SETTING PARAMETERS(R0 = 1, ...)
>
> This would make the R0 parameter optional, with a default value of
> 1. This is already implemented in my current development version. I
> guess a similar syntax will be implemented for instrument input
> parameters.
>
>  - Kristian.

--
Dr. Thomas C HANSEN, Instrument Scientist D20, Diffraction Group
Institut Max von Laue-Paul Langevin, BP 156, 38042 Grenoble C?dex 9, France
ILL4-1st floor room 100, Phone +33(0)476207044, Fax +33(0)476207648
mailto:hansen at ill.fr, http://www.ill.fr/YellowBook/D20
Private: 13, all?e des ?tangs, 38240 Meylan, France, +33(0)476180553


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Source_alpha=.1 	Source_beta=.1
Source_N_E=71		Source_N_xpos=1		Source_N_xdiv=1
Source_Lmin=2.3	Source_Lmax=2.5
Filter_d=0.05
Mono_position=17.2
Mono_omega=0
Mono_foccus=0.3
Mono_mosh=10		Mono_mosv=10
Mono_a=5.65		Mono_Vc=180.362
Mono_h0=3		Mono_k0=3		Mono_l0=5
Mono_h=1		Mono_k=1		Mono_l=3
Mono_F2=536.64		Mono_B=1
Mono_xmax=0.008		Mono_ymax=0.019		Mono_dist=0.020	Mono_zmax=0.07
Mono_blades=15
Mono_harmonic=3
Mono_LIMIT=10001
Takeoff=-90

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#0.700000 0.003500 0.050000 0.000100 # sample: packing radius height wall
#1.472205 0.153000 0.100000 0.053205 3.000000 # PSD: radius height pitch gap pressure
 160.176    1.368    0.032 # Si powder: Vc sig_a sig_i
24
   2.004   8            550.881     0.979320  1 1  1  1 
   3.272  12           1101.763     0.945799  1 2  2  0 
   4.008   8              0.000     0.919810  1 2  2  2 
   3.837  24            550.881     0.926239  1 3  1  1 
   5.043  24            550.880     0.876036  1 3  3  1 
   6.012   8            550.881     0.828554  1 3  3  3 
   4.628   6           1101.763     0.894535  1 4  0  0 
   5.668  24           1101.763     0.846050  1 4  2  2 
   6.545  12           1101.763     0.800193  1 4  4  0 
   6.942  24              0.000     0.778205  1 4  4  2 
   8.016   8           1101.763     0.715801  1 4  4  4 
   6.012  24            550.881     0.828554  1 5  1  1 
   6.845  48            550.881     0.783645  1 5  3  1 
   7.587  24            550.881     0.741170  1 5  3  3 
   8.262  24            550.882     0.700998  1 5  5  1 
   8.887  24            550.882     0.663003  1 5  5  3 
   7.317  24           1101.763     0.756822  1 6  2  0 
   7.674  24              0.000     0.736026  1 6  2  2 
   8.658  48           1101.763     0.677004  1 6  4  2 
   9.540  24              0.000     0.622715  1 6  4  4 
   8.262  24            550.882     0.700998  1 7  1  1 
   8.887  48            550.881     0.663003  1 7  3  1 
   9.470  24            550.883     0.627067  1 7  3  3 
   9.256   6           1101.763     0.640309  1 8  0  0 
  1889.494   133.139  19.677  YIG
  210 YIG
     0.719        12          0.000      0.998322
     1.016         6          0.000      0.996636
     1.245        24        203.580      0.984168
     1.438        12       3016.019      0.986776
     1.607        24          0.000      0.992151
     1.761         8          0.000      0.989722
     1.902        48       1506.029      0.978739
     2.033         6      98281.828      0.986199
     2.156        12          0.000      0.986071
     2.156        24          0.000      0.981520
     2.273        24      54691.691      0.986475
     2.384        24      36367.449      0.977947
     2.490        24      18260.684      0.979746
     2.592        48      13085.104      0.977365
     2.592        24          0.000      0.980939
     2.784        48       9884.264      0.981401
     2.875        12      11381.769      0.984795
     2.963        24          0.000      0.972488
     2.963        24          0.000      0.974189
     3.049        24          0.000      0.970052
     3.049         6          0.000      0.980046
     3.133        48       4738.101      0.980699
     3.133        24      26526.645      0.972831
     3.214        24      17280.061      0.952795
     3.294        48       1072.821      0.963691
     3.371        24          0.000      0.964791
     3.447        48       5640.986      0.945413
     3.521         8     108324.977      0.971225
     3.594        48        710.790      0.956927
     3.594        12          0.000      0.972702
     3.594        24          0.000      0.964389
     3.665        24     190097.016      0.960594
     3.735        24       8854.975      0.967531
     3.735        24       2605.230      0.928074
     3.735        48        136.468      0.844741
     3.803        48     127188.094      0.952464
     3.871        24          0.000      0.959452
     4.002        48         48.465      1.173685
     4.002        48      14212.914      0.934375
     4.066         6     244666.688      0.951433
     4.129        24          0.000      0.941082
     4.129        48       7215.575      0.943539
     4.129        24          0.000      0.937901
     4.191        24          0.000      0.946819
     4.191        24      17019.494      0.941878
     4.252        48       8083.322      0.921666
     4.313        12        734.671      1.049026
     4.313        24      10628.211      0.910545
     4.372        48       7646.340      0.936915
     4.372        24          0.000      0.915093
     4.372        48        776.047      0.936915
     4.431        24          0.000      0.930654
     4.489        48       8357.111      0.913423
     4.546        24      99628.523      0.932912
     4.602        24          0.000      0.925655
     4.602        24          0.000      0.927404
     4.658        48      41391.684      0.946833
     4.713        24       6454.844      0.952557
     4.713        48      20689.980      0.912980
     4.713        48       1554.205      0.876190
     4.768        24      82241.906      0.926566
     4.822        48      21384.988      0.923807
     4.822        48      15318.223      0.923807
     4.822        24          0.000      0.925684
     4.928        48        504.394      0.824814
     4.928        48         19.874      1.482843
     4.980        24      16359.466      0.889442
     5.031        12          0.000      0.922682
     5.031        48      39592.711      0.917322
     5.031        48      25325.520      0.917322
     5.082        24        129.762      0.915708
     5.082         6          0.000      0.924715
     5.133        24       1579.174      0.975029
     5.133        24      20095.832      0.897369
     5.183        48        673.349      1.077036
     5.183        24      43752.160      0.932161
     5.233        48      10300.698      0.910883
     5.233        24          0.000      0.893915
     5.282         8          0.000      0.903652
     5.282        24          0.000      0.903433
     5.330        48      11530.723      0.931612
     5.330        48        131.671      0.698822
     5.330        48       1564.328      0.844278
     5.426        24          0.000      0.903811
     5.426        24          0.000      0.911782
     5.426        48       5560.977      0.904489
     5.474        48      43032.797      0.926892
     5.474        24     121046.172      0.917166
     5.521        48        869.710      0.995956
     5.521        24       1071.323      0.986376
     5.567        48     100115.828      0.901113
     5.614        48       1334.206      0.898139
     5.614        48       1100.267      0.898139
     5.614        24          0.000      0.894209
     5.705        48         44.953      0.516079
     5.705        48      11047.518      0.922668
     5.705        48       4519.932      0.938451
     5.750        12     231623.359      0.905655
     5.795        24          0.000      0.898561
     5.795        24          0.000      0.895735
     5.839        24          0.000      0.902606
     5.839        24          0.000      0.884242
     5.883        24      24914.727      0.869469
     5.883        48       7679.861      0.854214
     5.883        48        125.314      1.182243
     5.883        48       1178.122      0.802006
     5.927        24       7067.095      0.950199
     5.927        24      11585.631      0.936204
     5.970        48        462.440      0.885574
     5.970        48       5778.562      0.885574
     6.014        48      22267.492      0.884016
     6.056        48        486.486      1.034189
     6.099        24      72231.336      0.882867
     6.099         6      19129.297      0.884716
     6.141        48         72.866      0.879357
     6.141        48      27934.947      0.879357
     6.141        48       5137.507      0.879357
     6.141        24          0.000      0.883748
     6.141        24          0.000      0.887918
     6.183        24      66256.578      0.901881
     6.225        24       1145.936      0.779438
     6.225        48       2368.012      0.946966
     6.225        48          2.107      0.093289
     6.266        48      84037.055      0.876638
     6.266        24     134249.734      0.876239
     6.307        48       1321.134      0.873184
     6.307        48      23028.475      0.873184
     6.388        48        378.576      0.698084
     6.388        48       1202.565      0.771261
     6.429        24       4163.282      0.777967
     6.469        24          0.000      0.847652
     6.469        12          0.000      0.913683
     6.469        48       1046.849      0.867055
     6.469        24          0.000      0.732765
     6.509        24          0.000      0.861072
     6.509        24      10020.346      0.865529
     6.509        48        100.722      0.865529
     6.548        48       5719.824      0.913443
     6.548        24      10481.625      0.900393
     6.548        48      34038.199      0.884106
     6.587        48       2212.532      0.734415
     6.627        48       8340.317      0.860968
     6.627        24          0.000      0.864604
     6.627        48       1144.634      0.860968
     6.627        24          0.000      0.866319
     6.665        24          0.000      0.861820
     6.704        48       4163.081      0.799453
     6.704        48       2879.308      0.931003
     6.704        48      18606.156      0.830018
     6.743        24      31417.455      0.935357
     6.781        24          0.000      0.851566
     6.781        48      19656.873      0.854924
     6.781        24          0.000      0.899097
     6.819        48     154874.438      0.872072
     6.819        24      45146.090      0.888126
     6.856        48          1.584      6.976236
     6.856        48         51.244      1.500796
     6.856        48       1127.712      0.974933
     6.894        48      50511.836      0.853395
     6.931        48      34190.152      0.848923
     6.931        48       2164.648      0.848923
     6.931        48        524.398      0.848923
     7.006        48      10537.984      0.806079
     7.042         8     279514.156      0.860435
     7.079        48       4450.304      0.842964
     7.079        48         91.726      0.842964
     7.079        24          0.000      0.833867
     7.079        48        236.346      0.842964
     7.079        48      13131.040      0.842964
     7.079        24          0.000      0.818209
     7.115        48       2832.459      0.841480
     7.115         6          0.000      0.853769
     7.152        24      55446.820      0.821886
     7.152        24      10563.778      0.798793
     7.152        48      29967.029      0.815409
     7.152        24        871.975      0.991503
     7.188        48       2430.303      0.697682
     7.188        12      61323.203      0.809452
     7.188        24      15699.059      0.781564
     7.223        24          0.000      0.866574
     7.223        48      26204.113      0.837046
     7.259        24          0.000      0.837881
     7.259        24          0.000      0.829693
     7.295        48      11099.855      0.792550
     7.295        48       1751.051      0.731513
     7.295        48       1620.526      0.947878
     7.295        48       5809.077      0.776945
     7.295        48       3604.480      0.909587
     7.330        24      73445.188      0.835414
     7.365        48      15921.470      0.831170
     7.365        48       5873.266      0.831170
     7.400        48      76166.891      0.860376
     7.400        24      54682.270      0.865962
     7.435        48      19258.697      0.795594
     7.435        24       2714.380      0.742726
     7.470        24     165646.812      0.828709
     7.470        24      74290.812      0.829656
     7.470        48     151288.562      0.828798
     7.504        48      10344.729      0.825335
     7.504        48       5411.900      0.825336
     7.504        24          0.000      0.822316
     7.573        48       1254.346      0.694604
     7.573        48        148.693      0.481002
     7.573        48      30448.402      0.795615
     7.607        48       1966.262      1.010599
     7.640        24          0.000      0.827541
     7.640        48       6363.631      0.819542
     7.640        24          0.000      0.837935
     7.674        24          0.000      0.824846
     7.674        24          0.000      0.818697
 160.176    1.368    0.032 Si
24
   2.004   8            550.837     0.940795 
   3.272  12           1101.675     0.849807 
   4.008   8              0.000     0.783395 
   3.837  24            550.837     0.799495 
   5.043  24            550.836     0.679416 
   6.012   8            550.837     0.577373 
   4.628   6           1101.675     0.722172 
   5.668  24           1101.675     0.613707 
   6.545  12           1101.675     0.521533 
   6.942  24              0.000     0.480775 
   8.016   8           1101.675     0.376637 
   6.012  24            550.837     0.577373 
   6.845  48            550.837     0.490656 
   7.587  24            550.837     0.416963 
   8.262  24            550.838     0.354338 
   8.887  24            550.838     0.301119 
   7.317  24           1101.675     0.443202 
   7.674  24              0.000     0.408566 
   8.658  48           1101.675     0.320069 
   9.540  24              0.000     0.250740 
   8.262  24            550.837     0.354338 
   8.887  48            550.836     0.301119 
   9.470  24            550.839     0.255893 
   9.256   6           1101.675     0.271997 
  24.265    5.120   0.800  Fe
10 Fe
   3.100  12            357.210     0.940960 1
   4.384   6            357.210     0.885405 1
   5.369  24            357.210     0.833130 1
   6.200  12            357.210     0.783942 1
   6.932  24            357.210     0.737658 1
   7.593   8            357.210     0.694106 1
   8.202  48            357.210     0.653126 1
   8.768   6            357.210     0.614565 1
   9.300  24            357.210     0.578281 1
   9.300  12            357.210     0.578281 1

-------------- next part --------------
# 0.600000 0.003500 0.050000 0.000100 # sample: packing radius height wall
# 1.472205 0.153000 0.100000 0.053205 3.000000 # PSD: radius height pitch gap pressure
  1889.494   133.139  19.677  # YIG powder: Vc sig_a sig_i
  400 YIG
        0.719           12        0.000     0.998322            1            1            0
        1.016            6        0.000     0.996636            2            0            0
        1.245           24      203.580     0.984168            2            1            1
        1.438           12     3016.019     0.986776            2            2            0
        1.607           24        0.000     0.992151            3            1            0
        1.761            8        0.000     0.989722            2            2            2
        1.902           48     1506.029     0.978739            3            2            1
        2.033            6    98281.828     0.986199            4            0            0
        2.156           12        0.000     0.986071            3            3            0
        2.156           24        0.000     0.981520            4            1            1
        2.273           24    54691.691     0.986475            4            2            0
        2.384           24    36367.449     0.977947            3            3            2
        2.490           24    18260.684     0.979746            4            2            2
        2.592           48    13085.104     0.977365            4            3            1
        2.592           24        0.000     0.980939            5            1            0
        2.784           48     9884.264     0.981401            5            2            1
        2.875           12    11381.769     0.984795            4            4            0
        2.963           24        0.000     0.972488            4            3            3
        2.963           24        0.000     0.974189            5            3            0
        3.049           24        0.000     0.970052            4            4            2
        3.049            6        0.000     0.980046            6            0            0
        3.133           48     4738.101     0.980699            5            3            2
        3.133           24    26526.645     0.972831            6            1            1
        3.214           24    17280.061     0.952795            6            2            0
        3.294           48     1072.821     0.963691            5            4            1
        3.371           24        0.000     0.964791            6            2            2
        3.447           48     5640.986     0.945413            6            3            1
        3.521            8   108324.977     0.971225            4            4            4
        3.594           48      710.790     0.956927            5            4            3
        3.594           12        0.000     0.972702            5            5            0
        3.594           24        0.000     0.964389            7            1            0
        3.665           24   190097.016     0.960594            6            4            0
        3.735           24     8854.975     0.967531            5            5            2
        3.735           24     2605.230     0.928074            6            3            3
        3.735           48      136.468     0.844741            7            2            1
        3.803           48   127188.094     0.952464            6            4            2
        3.871           24        0.000     0.959452            7            3            0
        4.002           48       48.465     1.173685            6            5            1
        4.002           48    14212.914     0.934375            7            3            2
        4.066            6   244666.688     0.951433            8            0            0
        4.129           24        0.000     0.941082            5            5            4
        4.129           48     7215.575     0.943539            7            4            1
        4.129           24        0.000     0.937901            8            1            1
        4.191           24        0.000     0.946819            6            4            4
        4.191           24    17019.494     0.941878            8            2            0
        4.252           48     8083.322     0.921666            6            5            3
        4.313           12      734.671     1.049026            6            6            0
        4.313           24    10628.211     0.910545            8            2            2
        4.372           48     7646.340     0.936915            7            4            3
        4.372           24        0.000     0.915093            7            5            0
        4.372           48      776.047     0.936915            8            3            1
        4.431           24        0.000     0.930654            6            6            2
        4.489           48     8357.111     0.913423            7            5            2
        4.546           24    99628.523     0.932912            8            4            0
        4.602           24        0.000     0.925655            8            3            3
        4.602           24        0.000     0.927404            9            1            0
        4.658           48    41391.684     0.946833            8            4            2
        4.713           24     6454.844     0.952557            6            5            5
        4.713           48    20689.980     0.912980            7            6            1
        4.713           48     1554.205     0.876190            9            2            1
        4.768           24    82241.906     0.926566            6            6            4
        4.822           48    21384.988     0.923807            7            5            4
        4.822           48    15318.223     0.923807            8            5            1
        4.822           24        0.000     0.925684            9            3            0
        4.928           48      504.394     0.824814            7            6            3
        4.928           48       19.874     1.482843            9            3            2
        4.980           24    16359.466     0.889442            8            4            4
        5.031           12        0.000     0.922682            7            7            0
        5.031           48    39592.711     0.917322            8            5            3
        5.031           48    25325.520     0.917322            9            4            1
        5.082           24      129.762     0.915708            8            6            0
        5.082            6        0.000     0.924715           10            0            0
        5.133           24     1579.174     0.975029            7            7            2
        5.133           24    20095.832     0.897369           10            1            1
        5.183           48      673.349     1.077036            8            6            2
        5.183           24    43752.160     0.932161           10            2            0
        5.233           48    10300.698     0.910883            9            4            3
        5.233           24        0.000     0.893915            9            5            0
        5.282            8        0.000     0.903652            6            6            6
        5.282           24        0.000     0.903433           10            2            2
        5.330           48    11530.723     0.931612            7            6            5
        5.330           48      131.671     0.698822            9            5            2
        5.330           48     1564.328     0.844278           10            3            1
        5.426           24        0.000     0.903811            7            7            4
        5.426           24        0.000     0.911782            8            5            5
        5.426           48     5560.977     0.904489            8            7            1
        5.474           48    43032.797     0.926892            8            6            4
        5.474           24   121046.172     0.917166           10            4            0
        5.521           48      869.710     0.995956            9            6            1
        5.521           24     1071.323     0.986376           10            3            3
        5.567           48   100115.828     0.901113           10            4            2
        5.614           48     1334.206     0.898139            8            7            3
        5.614           48     1100.267     0.898139            9            5            4
        5.614           24        0.000     0.894209           11            1            0
        5.705           48       44.953     0.516079            9            6            3
        5.705           48    11047.518     0.922668           10            5            1
        5.705           48     4519.932     0.938451           11            2            1
        5.750           12   231623.359     0.905655            8            8            0
        5.795           24        0.000     0.898561            9            7            0
        5.795           24        0.000     0.895735           11            3            0
        5.839           24        0.000     0.902606            8            8            2
        5.839           24        0.000     0.884242           10            4            4
        5.883           24    24914.727     0.869469            7            7            6
        5.883           48     7679.861     0.854214            9            7            2
        5.883           48      125.314     1.182243           10            5            3
        5.883           48     1178.122     0.802006           11            3            2
        5.927           24     7067.095     0.950199            8            6            6
        5.927           24    11585.631     0.936204           10            6            0
        5.970           48      462.440     0.885574            8            7            5
        5.970           48     5778.562     0.885574           11            4            1
        6.014           48    22267.492     0.884016           10            6            2
        6.056           48      486.486     1.034189            9            6            5
        6.099           24    72231.336     0.882867            8            8            4
        6.099            6    19129.297     0.884716           12            0            0
        6.141           48       72.866     0.879357            9            7            4
        6.141           48    27934.947     0.879357            9            8            1
        6.141           48     5137.507     0.879357           11            4            3
        6.141           24        0.000     0.883748           11            5            0
        6.141           24        0.000     0.887918           12            1            1
        6.183           24    66256.578     0.901881           12            2            0
        6.225           24     1145.936     0.779438           10            5            5
        6.225           48     2368.012     0.946966           10            7            1
        6.225           48        2.107     0.093289           11            5            2
        6.266           48    84037.055     0.876638           10            6            4
        6.266           24   134249.734     0.876239           12            2            2
        6.307           48     1321.134     0.873184            9            8            3
        6.307           48    23028.475     0.873184           12            3            1
        6.388           48      378.576     0.698084           10            7            3
        6.388           48     1202.565     0.771261           11            6            1
        6.429           24     4163.282     0.777967           12            4            0
        6.469           24        0.000     0.847652            8            7            7
        6.469           12        0.000     0.913683            9            9            0
        6.469           48     1046.849     0.867055           11            5            4
        6.469           24        0.000     0.732765           12            3            3
        6.509           24        0.000     0.861072            8            8            6
        6.509           24    10020.346     0.865529           10            8            0
        6.509           48      100.722     0.865529           12            4            2
        6.548           48     5719.824     0.913443            9            7            6
        6.548           24    10481.625     0.900393            9            9            2
        6.548           48    34038.199     0.884106           11            6            3
        6.587           48     2212.532     0.734415           10            8            2
        6.627           48     8340.317     0.860968            9            8            5
        6.627           24        0.000     0.864604           11            7            0
        6.627           48     1144.634     0.860968           12            5            1
        6.627           24        0.000     0.866319           13            1            0
        6.665           24        0.000     0.861820           10            6            6
        6.704           48     4163.081     0.799453           10            7            5
        6.704           48     2879.308     0.931003           11            7            2
        6.704           48    18606.156     0.830018           13            2            1
        6.743           24    31417.455     0.935357           12            4            4
        6.781           24        0.000     0.851566            9            9            4
        6.781           48    19656.873     0.854924           12            5            3
        6.781           24        0.000     0.899097           13            3            0
        6.819           48   154874.438     0.872072           10            8            4
        6.819           24    45146.090     0.888126           12            6            0
        6.856           48        1.584     6.976236           10            9            1
        6.856           48       51.244     1.500796           11            6            5
        6.856           48     1127.712     0.974933           13            3            2
        6.894           48    50511.836     0.853395           12            6            2
        6.931           48    34190.152     0.848923           11            7            4
        6.931           48     2164.648     0.848923           11            8            1
        6.931           48      524.398     0.848923           13            4            1
        7.006           48    10537.984     0.806079           10            9            3
        7.042            8   279514.156     0.860435            8            8            8
        7.079           48     4450.304     0.842964            9            8            7
        7.079           48       91.726     0.842964           11            8            3
        7.079           24        0.000     0.833867           12            5            5
        7.079           48      236.346     0.842964           12            7            1
        7.079           48    13131.040     0.842964           13            4            3
        7.079           24        0.000     0.818209           13            5            0
        7.115           48     2832.459     0.841480           12            6            4
        7.115            6        0.000     0.853769           14            0            0
        7.152           24    55446.820     0.821886            9            9            6
        7.152           24    10563.778     0.798793           10            7            7
        7.152           48    29967.029     0.815409           13            5            2
        7.152           24      871.975     0.991503           14            1            1
        7.188           48     2430.303     0.697682           10            8            6
        7.188           12    61323.203     0.809452           10           10            0
        7.188           24    15699.059     0.781564           14            2            0
        7.223           24        0.000     0.866574           11            9            0
        7.223           48    26204.113     0.837046           12            7            3
        7.259           24        0.000     0.837881           10           10            2
        7.259           24        0.000     0.829693           14            2            2
        7.295           48    11099.855     0.792550           10            9            5
        7.295           48     1751.051     0.731513           11            7            6
        7.295           48     1620.526     0.947878           11            9            2
        7.295           48     5809.077     0.776945           13            6            1
        7.295           48     3604.480     0.909587           14            3            1
        7.330           24    73445.188     0.835414           12            8            0
        7.365           48    15921.470     0.831170           11            8            5
        7.365           48     5873.266     0.831170           13            5            4
        7.400           48    76166.891     0.860376           12            8            2
        7.400           24    54682.270     0.865962           14            4            0
        7.435           48    19258.697     0.795594           13            6            3
        7.435           24     2714.380     0.742726           14            3            3
        7.470           24   165646.812     0.828709           10           10            4
        7.470           24    74290.812     0.829656           12            6            6
        7.470           48   151288.562     0.828798           14            4            2
        7.504           48    10344.729     0.825335           11            9            4
        7.504           48     5411.900     0.825336           12            7            5
        7.504           24        0.000     0.822316           13            7            0
        7.573           48     1254.346     0.694604           11           10            1
        7.573           48      148.693     0.481002           13            7            2
        7.573           48    30448.402     0.795615           14            5            1
        7.607           48     1966.262     1.010599           12            8            4
        7.640           24        0.000     0.827541            9            9            8
        7.640           48     6363.631     0.819542           12            9            1
        7.640           24        0.000     0.837935           15            1            0
        7.674           24        0.000     0.824846           10            8            8
        7.674           24        0.000     0.818697           14            4            4
        7.708           48     3849.914     0.896828           10            9            7
        7.708           48     1094.647     0.676433           11           10            3
        7.708           48       79.345     0.362349           13            6            5
        7.708           48       79.048     1.454426           14            5            3
        7.708           48     5521.893     0.883341           15            2            1
        7.741           24       74.444     0.141779           14            6            0
        7.775           48    15044.647     0.813789           11            8            7
        7.775           48    11309.317     0.813789           12            9            3
        7.775           48    14739.329     0.813789           13            7            4
        7.775           48     3247.167     0.813789           13            8            1
        7.775           24        0.000     0.828548           15            3            0
        7.808           24        0.000     0.844919           10           10            6
        7.808           48    11997.312     0.812357           14            6            2
        7.841           48    19856.273     0.775865           11            9            6
        7.841           48    13406.674     0.854643           15            3            2
        7.906           12        0.000     0.816166           11           11            0
        7.906           24        0.000     0.830149           12            7            7
        7.906           48     7061.392     0.808076           13            8            3
        7.906           48     2060.587     0.808076           15            4            1
        7.939           48    93269.773     0.837780           12            8            6
        7.939           24    47890.504     0.850255           12           10            0
        7.971           48     7796.717     0.748176           11           10            5
        7.971           24     7086.558     0.745438           11           11            2
        7.971           24     2328.366     0.702413           14            5            5
        7.971           48       19.962     0.066294           14            7            1
        8.004           48   112340.125     0.806478           12           10            2
        8.004           48    53296.637     0.807681           14            6            4
        8.036           48    14131.926     0.802403           12            9            5
        8.036           24        0.000     0.829866           13            9            0
        8.036           48      956.852     0.802403           15            4            3
        8.036           24        0.000     0.785195           15            5            0
        8.100           48      125.046     1.339667           13            7            6
        8.100           48     2835.213     0.703768           13            9            2
        8.100           48       10.602     0.000098           14            7            3
        8.100           48     1178.623     0.653589           15            5            2
        8.132            6   151833.891     0.825886           16            0            0
        8.163           24        0.000     0.795598           11           11            4
        8.163           48     1550.868     0.796771           13            8            5
        8.163           24        0.000     0.872871           16            1            1
        8.195           48      242.107     0.795369           12           10            4
        8.195           24    33236.344     0.795369           14            8            0
        8.195           24    34660.660     0.795369           16            2            0
        8.227           24    12606.899     0.842757           10            9            9
        8.227           48     2381.923     0.687250           15            6            1
        8.258           24      864.789     0.513735           10           10            8
        8.258           48     6570.184     0.908619           14            8            2
        8.258           24     6778.777     0.906760           16            2            2
        8.289           48      966.176     0.791177           11            9            8
        8.289           48    43581.391     0.791178           12           11            1
        8.289           48     7196.764     0.791178           13            9            4
        8.289           48    10670.142     0.791177           15            5            4
        8.289           48     3204.440     0.791177           16            3            1
        8.320           24        0.000     0.808097           14            6            6
        8.351           48      200.804     1.226601           11           10            7
        8.351           48     2200.392     0.910606           13           10            1
        8.351           48     1091.037     0.629967           14            7            5
        8.351           48     3256.225     0.888213           15            6            3
        8.382           24    93462.555     0.790193           12            8            8
        8.382           24    75682.148     0.790548           16            4            0
        8.413           48    11445.481     0.785624           12            9            7
        8.413           48      142.793     0.785624           12           11            3
        8.413           24        0.000     0.807413           15            7            0
        8.413           24        0.000     0.793343           16            3            3
        8.443           48    66963.406     0.824903           14            8            4
        8.443           48   152509.391     0.811070           16            4            2
        8.474           24      991.613     0.613598           11           11            6
        8.474           48     1375.104     0.637806           13           10            3
        8.474           48     3873.620     0.694648           14            9            1
        8.474           48     6604.764     0.853982           15            7            2
        8.504           48   105229.992     0.784568           12           10            6
        8.535           48    20650.426     0.780109           13            8            7
        8.535           48    11068.548     0.780109           16            5            1
        8.595           48     1777.985     0.920500           13            9            6
        8.595           48     9026.879     0.839398           14            9            3
        8.595           48     1867.975     0.649371           15            6            5
        8.625           12      440.601     0.382222           12           12            0
        8.625           24     4123.180     0.934647           16            4            4
        8.655           48     2586.402     0.774632           12           11            5
        8.655           24        0.000     0.773600           13           11            0
        8.655           48        3.233     0.774635           15            7            4
        8.655           48    53071.383     0.774632           15            8            1
        8.655           48     3789.377     0.774632           16            5            3
        8.655           24        0.000     0.795470           17            1            0
        8.685           24        0.000     0.771895           12           12            2
        8.685           24     3643.341     0.773269           16            6            0
        8.714           48      941.143     0.591423           13           10            5
        8.714           48     3285.156     0.878372           13           11            2
        8.714           24    39280.148     0.801991           14            7            7
        8.714           48     8748.503     0.710066           17            2            1
        8.744           48     1214.614     0.512271           14            8            6
        8.744           24     2282.333     0.576950           14           10            0
        8.744           48       57.059     2.642583           16            6            2
        8.773           48      308.901     0.769195           15            8            3
        8.773           24        0.000     0.819555           17            3            0
        8.803            8        0.000     0.755858           10           10           10
        8.803           48      454.897     0.767840           14           10            2
        8.832           48    12771.266     0.820756           11           10            9
        8.832           48     6171.375     0.845140           14            9            5
        8.832           48      590.266     1.034670           17            3            2
        8.861           24   104101.289     0.832626           12           12            4
        8.890           24        0.000     0.770600           11           11            8
        8.890           24        0.000     0.675269           12            9            9
        8.890           48     9594.028     0.763795           13           11            4
        8.890           24        0.000     0.801700           15            9            0
        8.890           24        0.000     0.763028           16            5            5
        8.890           48    11653.093     0.763795           16            7            1
        8.890           48      960.200     0.763795           17            4            1
        8.919           48    41982.527     0.818643           12           10            8
        8.919           48    84537.617     0.801842           16            6            4
        8.948           48     1440.681     0.931723           15            7            6
        8.948           48     6684.949     0.687764           15            9            2
        8.977           48    31867.904     0.765981           14           10            4
        9.006           48     3182.443     0.758433           12           11            7
        9.006           48       58.134     0.758433           13            9            8
        9.006           48    11570.396     0.758433           13           12            1
        9.006           48     5064.502     0.758433           15            8            5
        9.006           48     6890.246     0.758433           16            7            3
        9.006           48    12437.841     0.758433           17            4            3
        9.006           24        0.000     0.781995           17            5            0
        9.063           48     2402.020     0.633288           13           10            7
        9.063           48      935.103     0.974633           14           11            1
        9.063           48     2552.169     0.636789           17            5            2
        9.092           24   489417.750     0.772806           16            8            0
        9.120           48    16024.504     0.753109           13           12            3
        9.120           48     2811.926     0.753109           15            9            4
        9.148           24        0.000     0.772726           12           12            6
        9.148           24        0.000     0.725124           14            8            8
        9.148           48     1665.530     0.751784           16            8            2
        9.148            6        0.000     0.769562           18            0            0
        9.176           48    13771.264     0.697036           13           11            6
        9.176           48    29490.500     0.713739           14            9            7
        9.176           48    15184.293     0.699537           14           11            3
        9.176           48     1268.854     0.940422           15           10            1
        9.176           48      229.789     0.388343           17            6            1
        9.176           24     5101.780     0.663727           18            1            1
        9.205           24    26858.607     0.685284           16            6            6
        9.205           24     1676.267     1.033228           18            2            0
        9.233           48     4989.955     0.747822           16            7            5
        9.233           48    25568.219     0.747822           17            5            4
        9.260           48    15964.095     0.746507           14           10            6
        9.260           24        0.000     0.738002           18            2            2
        9.288           48     4842.825     0.841539           15           10            3
        9.288           48       59.952     1.821303           17            6            3
        9.288           48      842.021     0.986068           18            3            1
        9.316           48    73451.273     0.748262           16            8            4
        9.344           48     1779.935     0.742573           13           12            5
        9.344           12        0.000     0.750385           13           13            0
        9.344           48     7446.031     0.742573           15            8            7
        9.344           48       64.178     0.742571           16            9            1
        9.344           24        0.000     0.721414           17            7            0
        9.371           24   116010.547     0.777449           14           12            0
        9.371           24       84.167     2.662763           18            4            0
        9.399           24    16458.018     0.792424           11           11           10
        9.399           24       25.086     2.650020           13           13            2
        9.399           48     4530.413     0.841504           14           11            5
        9.399           48    16069.531     0.793065           15            9            6
        9.399           48      967.204     0.542545           17            7            2
        9.399           24    13988.126     0.796950           18            3            3
        9.426           24    37421.613     0.744935           12           10           10
        9.426           48    39291.531     0.744784           14           12            2
        9.426           48    52253.723     0.743969           18            4            2
        9.454           48     8956.533     0.737360           12           11            9
        9.454           24        0.000     0.769230           15           11            0
        9.454           48     6119.978     0.737360           16            9            3
        9.508           48      367.693     0.425812           13           10            9
        9.508           48      205.257     1.279353           15           10            5
        9.508           48    18085.365     0.685595           15           11            2
        9.508           48    47413.023     0.704197           17            6            5
        9.508           48    11488.113     0.673343           18            5            1
        9.535           24     2087.741     0.507875           12           12            8
        9.562           48        8.731     0.732185           13           11            8
        9.562           24        0.000     0.730241           13           13            4
        9.562           24        0.000     0.779491           16            7            7
        9.562           48     7435.995     0.732184           17            7            4
        9.562           48     4377.982     0.732184           17            8            1
        9.589           48       21.935     0.730896           14           12            4
        9.589           48      592.034     0.730895           16            8            6
        9.589           24    12893.613     0.730895           16           10            0
        9.589           24        0.000     0.733011           18            4            4
        9.616           24      394.922     0.426086           14            9            9
        9.616           48     1802.463     0.577434           18            5            3
        9.643           48      986.512     1.137751           14           10            8
        9.643           48     4248.782     0.563507           16           10            2
        9.643           24    10720.993     0.622106           18            6            0
        9.670           48    30420.504     0.727044           13           12            7
        9.670           48     6393.077     0.727044           15           11            4
        9.670           48     3875.861     0.727044           16            9            5
        9.670           48     9838.925     0.727044           17            8            3
        9.670           24        0.000     0.748096           19            1            0
        9.697           48     8127.695     0.725765           18            6            2
        9.723           48      770.210     0.495789           14           11            7
        9.723           48     2651.060     0.595845           14           13            1
        9.723           48    16128.882     0.670819           19            2            1
        9.776           48     3330.684     0.721940           15            9            8
        9.776           48      723.887     0.721940           15           12            1
        9.776           24        0.000     0.759183           17            9            0
        9.776           24        0.000     0.781093           19            3            0
        9.802           48     6867.757     0.886021           16           10            4
        9.829           24    35440.613     0.757362           13           13            6
        9.829           48    10398.315     0.790245           14           13            3
        9.829           48     6696.791     0.635780           15           10            7
        9.829           48     9738.723     0.792662           17            7            6
        9.829           48      285.456     1.197523           17            9            2
        9.829           24    14787.541     0.662560           18            5            5
        9.829           48      926.501     0.969829           18            7            1
        9.829           48     3458.568     0.844357           19            3            2
        9.855           48   101912.961     0.722259           14           12            6
        9.855           48    70842.172     0.723083           18            6            4
        9.881           48     4636.409     0.716873           15           12            3
        9.881           48      871.953     0.716872           16           11            1
        9.881           48     2569.428     0.716873           17            8            5
        9.881           48       64.828     0.716872           19            4            1
        9.933           48     2296.289     0.871588           15           11            6
        9.933           48     3882.000     0.833895           18            7            3
        9.959           24   429715.625     0.735588           16            8            8
        9.985           24        0.000     0.728021           12           11           11
        9.985           48     3829.123     0.711840           16            9            7
        9.985           48     2300.313     0.711840           16           11            3
        9.985           48     2157.346     0.711840           17            9            4
        9.985           48        5.185     0.711839           19            4            3
        9.985           24        0.000     0.731896           19            5            0
       10.011           24        0.000     0.729847           12           12           10
       10.011           24     8407.514     0.710588           18            8            0
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       10.037           48        0.061   333.109955           14           13            5
       10.037           48     5228.630     0.612431           17           10            1
       10.037           48    10274.168     0.639479           19            5            2
       10.063           12    11096.196     0.827805           14           14            0
       10.063           48      491.430     0.266939           16           10            6
       10.063           48      354.569     0.210751           18            8            2
       10.088           48    23376.588     0.706843           13           12            9
       10.088           48    33480.711     0.706843           15           12            5
       10.088           24        0.000     0.738399           15           13            0
       10.114           24        0.000     0.727591           14           10           10
       10.114           24        0.000     0.748768           14           14            2
       10.114           24        0.000     0.757605           18            6            6
       10.139           48     7466.300     0.621679           14           11            9
       10.139           48      990.249     0.957920           15           13            2
       10.139           48     1190.770     0.934025           17           10            3
       10.139           48        9.645     0.329466           18            7            5
       10.139           48     8873.878     0.784734           19            6            1
       10.165           24   135888.438     0.706895           16           12            0
       10.165            6   200452.516     0.706227           20            0            0
       10.190           24        0.000     0.702737           13           13            8
       10.190           48    12294.665     0.701881           16           11            5
       10.190           48     5908.372     0.701881           17            8            7
       10.190           48     3440.059     0.701881           19            5            4
       10.190           24        0.000     0.664889           20            1            1
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       10.215           48    78204.258     0.750741           16           12            2
       10.215           48   108975.664     0.742971           18            8            4
       10.215           24   200123.938     0.731759           20            2            0
       10.241           48    16443.350     0.642387           15           10            9
       10.241           48      821.729     0.463152           17            9            6
       10.241           48      183.235     0.256509           18            9            1
       10.241           48       11.070     4.744914           19            6            3
       10.266           24    85986.914     0.703017           14           14            4
       10.266           24   176294.906     0.701557           20            2            2
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       10.291           24        0.000     0.705679           17           11            0
       10.291           24        0.000     0.727756           19            7            0
       10.291           48        7.288     0.696954           20            3            1
       10.341           48      211.520     1.312292           14           13            7
       10.341           48     1385.313     0.912704           17           10            5
       10.341           48    16359.064     0.636597           17           11            2
       10.341           48      490.017     0.394712           18            9            3
       10.341           48     6772.580     0.789503           19            7            2
       10.366           48     1908.914     0.434801           16           12            4
       10.366           24    23541.840     0.613565           20            4            0
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       10.391           24        0.000     0.799210           16            9            9
       10.391           24        0.000     0.729334           20            3            3
       10.416           48     6394.384     0.690844           16           10            8
       10.416           48     3046.540     0.690844           20            4            2
       10.440           48     2461.563     0.543780           15           14            1
       10.440           24      135.264     1.506200           18            7            7
       10.440           48    19656.266     0.636037           19            6            5
       10.465           48    22722.738     0.606361           18            8            6
       10.465           24    17729.400     0.595911           18           10            0
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       10.490           48      448.920     0.687203           16           13            1
       10.490           48     8295.166     0.687203           17           11            4
       10.490           48      139.147     0.687203           19            7            4
       10.490           48        0.328     0.687215           19            8            1
       10.490           48     3527.839     0.687203           20            5            1
       10.514           24        0.000     0.727619           14           14            6
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       10.539           48    26527.465     0.637960           15           14            3
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       10.563            8    52768.902     0.807684           12           12           12
       10.563           24    92219.422     0.776506           20            4            4
       10.588           48     5757.705     0.682379           13           12           11
       10.588           48     9340.360     0.682379           16           13            3
       10.588           48      710.295     0.682379           17            9            8
       10.588           48    10436.022     0.682379           17           12            1
       10.588           48    27884.703     0.682379           19            8            3
       10.588           48        5.528     0.682372           20            5            3
       10.612           48    62078.328     0.740588           16           12            6
       10.612           24     2835.733     0.980520           20            6            0
       10.637           24      336.916     1.175382           13           13           10
       10.637           24    33559.977     0.637768           14           11           11
       10.637           48      930.464     0.961942           17           10            7
       10.661           48    98878.328     0.683607           14           12           10
       10.661           48    42282.145     0.686166           18           10            4
       10.661           48    68886.531     0.684564           20            6            2
       10.685           48     1498.741     0.677589           17           12            3
       10.685           24        0.000     0.698189           19            9            0
       10.685           24        0.000     0.703940           21            1            0
       10.733           48     2054.250     0.511190           14           13            9
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       10.733           48     3496.692     0.547453           18           11            1
       10.733           48     5957.996     0.576137           19            7            6
       10.733           48     1422.699     0.480880           19            9            2
       10.733           48       29.973     2.908144           21            2            1
       10.781           48     1753.692     0.672832           15           12            9
       10.781           12        0.000     0.664564           15           15            0
       10.781           48     1753.916     0.672832           16           13            5
       10.781           48       40.492     0.672836           19            8            5
       10.781           24        0.000     0.690230           20            5            5
       10.781           48     3651.796     0.672833           20            7            1
       10.781           24        0.000     0.707799           21            3            0
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       10.805           48     9669.600     0.671649           20            6            4
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       10.829           48        7.145     1.037184           18            9            7
       10.829           48     5454.835     0.565999           18           11            3
       10.829           48    11229.632     0.748505           21            3            2
       10.853           24    15315.414     0.565674           14           14            8
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       10.853           48     3599.667     0.465110           16           14            2
       10.877           48    18971.936     0.668109           15           13            8
       10.877           48     6143.480     0.668110           16           11            9
       10.877           48     6768.690     0.668109           17           12            5
       10.877           24        0.000     0.688241           17           13            0
       10.877           48    21970.449     0.668109           19            9            4
       10.877           48     6369.703     0.668110           20            7            3
       10.877           48     1052.865     0.668110           21            4            1
       10.900           48     3017.939     0.666934           18           10            6
       10.924           48    19252.697     0.725662           17           13            2
       10.924           48    25930.057     0.616213           19           10            1
       10.948           48    84530.609     0.670057           16           12            8
       10.948           24    97406.680     0.669681           20            8            0
       10.971           24        0.000     0.685600           15           15            4
       10.971           48    10599.709     0.663419           21            4            3
       10.971           24        0.000     0.643299           21            5            0
       10.995           48   100173.562     0.711064           16           14            4
       10.995           24   166767.672     0.699932           18           12            0
       10.995           48   159852.547     0.700750           20            8            2
       11.018           48     1658.682     0.878372           15           14            7
       11.018           48    17370.697     0.600177           17           10            9
       11.018           48      597.529     0.367525           18           11            5
       11.018           48      997.503     0.426396           19           10            3
       11.018           48     3084.364     0.521335           21            5            2
       11.042           48   106769.031     0.664861           18           12            2
       11.042           24   137048.594     0.664281           20            6            6
       11.065           48     2199.089     0.658762           16           13            7
       11.065           48    22348.607     0.658762           17           11            8
       11.065           48     5517.560     0.658762           17           13            4
       11.065           48     2181.360     0.658762           19            8            7
       11.065           48      792.531     0.658762           20            7            5
       11.112           48       94.408     1.790153           19            9            6
       11.112           48     8604.981     0.749077           21            6            1
       11.135           48    12669.628     0.783483           20            8            4
       11.158           24        0.000     0.646298           13           13           12
       11.158           48     9421.717     0.654138           16           15            1
       11.158           48      210.036     0.654139           17           12            7
       11.158           24        0.000     0.710653           19           11            0
       11.158           48       92.088     0.654137           20            9            1
       11.158           48     2810.931     0.654138           21            5            4
       11.181           24        0.000     0.727377           14           12           12
       11.181           48     5305.505     0.652987           18           12            4
       11.181            6        0.000     0.654133           22            0            0
       11.204           48    15691.037     0.720583           14           13           11
       11.204           24    33526.344     0.606793           15           15            6
       11.204           48     3536.515     0.800657           17           14            1
       11.204           24      287.097     0.250511           18            9            9
       11.204           48     7806.454     0.750322           19           10            5
       11.204           48      812.864     0.390627           19           11            2
       11.204           48     8561.631     0.745729           21            6            3
       11.204           24    20528.598     0.594559           22            1            1
       11.227           48       14.069     2.231752           16           14            6
       11.227           48     3712.752     0.899219           18           10            8
       11.227           24      759.892     1.253699           22            2            0
       11.250           48      487.995     0.649546           15           12           11
       11.250           48     2527.021     0.649546           16           15            3
       11.250           48     4456.323     0.649545           20            9            3
       11.250           24        0.000     0.652303           21            7            0
       11.273           24        0.000     0.789600           14           14           10
       11.273           24        0.000     0.653409           22            2            2
       11.296           48      706.681     0.367562           15           13           10
       11.296           48      297.195     0.248811           17           13            6
       11.296           48     7711.250     0.554293           17           14            3
       11.296           48     2570.974     0.490818           18           11            7
       11.296           48     8067.584     0.745120           18           13            1
       11.296           48    22961.691     0.704436           21            7            2
       11.296           48       87.333     0.057870           22            3            1
       11.342           24        0.000     0.685507           16           11           11
       11.342           48      332.649     0.644986           19           11            4
       11.342           24        0.000     0.746241           20            7            7
       11.364           48   159977.438     0.683996           16           12           10
       11.364           48   130867.500     0.688308           20            8            6
       11.364           24    72803.609     0.703794           20           10            0
       11.364           24    23748.637     0.750559           22            4            0
       11.387           48     1212.476     0.912182           15           14            9
       11.387           48       14.392     4.882132           18           13            3
       11.387           48     1769.587     0.455264           21            6            5
       11.387           24    51470.301     0.681020           22            3            3
       11.410           48    99131.141     0.647012           18           12            6
       11.410           48    29163.473     0.651607           20           10            2
       11.410           48    92906.383     0.647192           22            4            2
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       11.432           48     4368.299     0.640459           16           15            5
       11.432           48    31403.549     0.640459           19            9            8
       11.432           48      119.824     0.640458           19           12            1
       11.432           48     2748.602     0.640458           20            9            5
       11.432           48      346.130     0.640457           21            7            4
       11.432           48     8339.304     0.640458           21            8            1
       11.478           48     5003.653     0.521834           17           11           10
       11.478           48     3454.537     0.793780           17           14            5
       11.478           48     4331.639     0.776329           19           10            7
       11.478           48      503.373     0.311025           22            5            1
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       11.522           48    13001.710     0.635962           17           12            9
       11.522           24        0.000     0.631716           17           15            0
       11.522           48     1780.457     0.635963           19           12            3
       11.522           48     6706.062     0.635963           21            8            3
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       11.545           24        0.000     0.604006           16           16            2
       11.545           48     8097.510     0.634843           20           10            4
       11.545           24        0.000     0.657954           22            4            4
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       11.567           48     8971.104     0.729207           18           13            5
       11.567           48     7212.025     0.535136           19           11            6
       11.567           48     5994.438     0.526029           22            5            3
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       11.590           24      518.950     0.157468           22            6            0
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       11.612           48     2803.506     0.631498           20           11            1
       11.612           24        0.000     0.667525           21            9            0
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       11.634           48    22130.412     0.630387           18           14            2
       11.634           48     1981.995     0.630388           22            6            2
       11.656           48      116.182     0.077477           18           11            9
       11.656           48    11704.309     0.550516           21            7            6
       11.656           48     4335.886     0.502654           21            9            2
       11.678           24   116167.578     0.633385           16           16            4
       11.678           24   107535.102     0.633591           20            8            8
       11.700           48     4930.005     0.627065           16           15            7
       11.700           48     4708.191     0.627065           17           15            4
       11.700           48    28224.625     0.627065           19           12            5
       11.700           24        0.000     0.596998           19           13            0
       11.700           48     2646.947     0.627066           20            9            7
       11.700           48      918.285     0.627066           20           11            3
       11.700           48     9310.486     0.627065           21            8            5
       11.700           24        0.000     0.611802           23            1            0
       11.723           48    74428.492     0.687569           18           12            8
       11.745           24    36005.445     0.578920           14           13           13
       11.745           48    21234.656     0.565384           17           14            7
       11.745           48     5825.659     0.746672           19           13            2
       11.745           24    23817.857     0.568623           22            5            5
       11.745           48     2404.847     0.819144           22            7            1
       11.745           48    14864.012     0.554119           23            2            1
       11.766           24   117187.000     0.629019           14           14           12
       11.766           48   163276.672     0.628214           18           14            4
       11.766           48    51583.629     0.631695           20           10            6
       11.766           48    66068.156     0.630769           22            6            4
       11.788           48     2424.192     0.622663           15           13           12
       11.788           48    12175.204     0.622663           21            9            4
       11.788           24        0.000     0.684423           23            3            0
       11.832           48     5088.439     0.752444           15           14           11
       11.832           48      461.719     0.273537           18           13            7
       11.832           48        9.878     6.746250           19           10            9
       11.832           48    13722.126     0.546340           21           10            1
       11.832           48     9360.422     0.716544           22            7            3
       11.832           48      285.144     0.203293           23            3            2
       11.854           24      245.206     1.926058           16           12           12
       11.854           24     5207.864     0.841583           20           12            0
       11.876           48     2550.054     0.618292           16           13           11
       11.876           48     1977.929     0.618292           17           16            1
       11.876           48    31793.830     0.618292           19           11            8
       11.876           48     2590.990     0.618292           19           13            4
       11.876           48     4312.363     0.618292           20           11            5
       11.876           48       68.349     0.618293           23            4            1
       11.897           24        0.000     0.601473           16           16            6
       11.897           48      325.180     0.617205           20           12            2
       11.897           24     7184.949     0.617204           22            8            0
       11.919           24     2757.569     0.800199           15           15           10
       11.919           48     6327.436     0.507762           17           15            6
       11.919           48     4055.922     0.482407           18           15            1
       11.919           48      242.952     0.172778           21           10            3
       11.941           48     7888.565     0.458459           16           14           10
       11.941           48      109.173     2.873094           22            8            2
       11.962           48    10852.533     0.613952           17           12           11
       11.962           48    16083.902     0.613952           17           16            3
       11.962           48    21445.627     0.613952           19           12            7
       11.962           48        1.472     0.613933           21            8            7
       11.962           48    37939.918     0.613952           23            4            3
       11.962           24        0.000     0.616921           23            5            0
       11.984           48     1296.799     0.612872           18           14            6
       11.984           24        0.000     0.712688           22            6            6
       12.006           48       82.405     2.026851           17           13           10
       12.006           48    18215.365     0.546157           18           15            3
       12.006           48     9411.382     0.709300           19           14            1
       12.006           48     2181.693     0.822372           21            9            6
       12.006           48      335.092     1.210647           22            7            5
       12.006           48     8659.716     0.517815           23            5            2
       12.027           48    95207.109     0.718642           20           12            4
       12.048           48       62.905     0.609640           16           15            9
       12.048           24        0.000     0.614455           20            9            9
       12.048           24        0.000     0.621012           21           11            0
       12.070           48    20326.646     0.733442           20           10            8
       12.070           48   105682.531     0.661900           22            8            4
       12.091           48    21634.326     0.671532           17           14            9
       12.091           24      972.384     0.937657           18           11           11
       12.091           48     1994.939     0.830481           19           13            6
       12.091           48        0.028  1184.492188           19           14            3
       12.091           48     3860.352     0.764279           21           10            5
       12.091           48     3519.251     0.462570           21           11            2
       12.091           48      775.554     0.981970           22            9            1
       12.091           48    10175.889     0.519880           23            6            1
       12.113           48    76630.094     0.613261           18           12           10
       12.134           48     3683.249     0.605362           17           16            5
       12.134           48     3521.664     0.605362           20           11            7
       12.134           48      124.058     0.605363           20           13            1
       12.134           48     3462.126     0.605362           23            5            4
       12.176           48       55.890     0.000408           18           13            9
       12.176           48       97.423     1.905106           18           15            5
       12.176           48    14498.582     0.528827           22            9            3
       12.176           48     4836.832     0.477510           23            6            3
       12.198           24   146829.391     0.652999           16           16            8
       12.198            6    48972.145     0.691485           24            0            0
       12.219           48     2249.633     0.601113           17           15            8
       12.219           12        0.000     0.648104           17           17            0
       12.219           48      731.749     0.601113           20           13            3
       12.219           48     2019.349     0.601113           21           11            4
       12.219           24        0.000     0.620825           23            7            0
       12.219           24        0.000     0.585538           24            1            1
       12.240           24     2309.716     0.600055           18           16            0
       12.240           48    12503.156     0.600055           20           12            6
       12.240           24      392.155     0.600055           24            2            0
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       12.261           48     1170.735     0.357480           19           11           10
       12.261           48     3571.711     0.453139           19           14            5
       12.261           24    23870.430     0.540168           22            7            7
       12.261           48    11697.327     0.515888           23            7            2
       12.282           48     1961.352     0.301177           18           14            8
       12.282           48     2399.438     0.325265           18           16            2
       12.282           48     8974.643     0.446666           22            8            6
       12.282           24    20183.016     0.494621           22           10            0
       12.282           24     4232.669     0.857612           24            2            2
       12.303           48     8762.402     0.596893           19           12            9
       12.303           24        0.000     0.652194           19           15            0
       12.303           48    16475.064     0.596893           21            9            8
       12.303           48    21749.035     0.596893           21           12            1
       12.303           48        0.566     0.596886           24            3            1
       12.324            8        0.000     0.643371           14           14           14
       12.324           48    12293.235     0.595843           22           10            2
       12.345           48      147.154     1.621171           15           14           13
       12.345           48     1708.446     0.389242           19           15            2
       12.345           48      516.791     1.079764           21           10            7
       12.345           48    11336.400     0.509842           22            9            5
       12.345           48    18111.604     0.527044           23            6            5
       12.366           24    58389.941     0.601851           24            4            0
       12.387           24        0.000     0.671713           15           15           12
       12.387           24        0.000     0.735260           16           13           13
       12.387           48    12095.004     0.592703           17           16            7
       12.387           24        0.000     0.624602           17           17            4
       12.387           48     6109.655     0.592703           19           13            8
       12.387           48     1167.612     0.592703           20           13            5
       12.387           48      486.571     0.592703           21           12            3
       12.387           48      968.762     0.592702           23            7            4
       12.387           48     2560.149     0.592703           23            8            1
       12.387           24        0.000     0.590848           24            3            3
       12.408           48    33698.273     0.690808           16           14           12
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       12.449           48    57275.621     0.597853           22           10            4
       12.470           48      789.999     0.588542           16           15           11
       12.470           48    10761.667     0.588542           17           13           12
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       12.470           48     3639.900     0.588543           23            8            3
       12.470           48    17676.646     0.588542           24            5            1
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       12.511           48    15084.020     0.511461           22           11            1
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       12.532           24     2797.412     0.326392           24            4            4
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       12.552           24        0.000     0.614612           23            9            0
       12.552           48     1401.835     0.584411           24            5            3
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       12.573           24        0.000     0.574667           18           12           12
       12.573           48       27.689     0.583384           20           14            4
       12.573           24        0.000     0.593523           22            8            8
       12.573           24      974.674     0.583382           24            6            0
       12.594           48     7713.880     0.696704           17           15           10
       12.594           24      625.189     0.261879           17           17            6
       12.594           48      342.001     0.179135           18           13           11
       12.594           48     2097.192     0.810675           18           17            1
       12.594           48      486.338     1.098598           21           13            2
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       12.594           48      257.410     0.137906           22           11            3
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       12.594           48     2041.253     0.814043           23            9            2
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       12.614           48     1627.606     1.038560           24            6            2
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       12.635           48     4582.844     0.580308           20           13            7
       12.635           48      424.410     0.580309           23            8            5
       12.655           48    31903.266     0.579287           18           14           10
       12.655           48     5253.120     0.579288           22           10            6
       12.675           48     2611.902     0.404740           18           17            3
       12.675           48    13236.974     0.497375           19           15            6
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       12.716           48     6512.263     0.576235           19           12           11
       12.716           48     7935.641     0.576235           19           16            3
       12.716           48     1384.119     0.576235           20           15            1
       12.716           48     6295.197     0.576235           21           11            8
       12.716           48    24718.215     0.576235           21           13            4
       12.716           48     5930.177     0.576235           23            9            4
       12.716           24        0.000     0.586224           24            5            5
       12.716           48    14408.281     0.576235           24            7            1
       12.716           24        0.000     0.599632           25            1            0
       12.736           24   120591.719     0.628172           22           12            0
       12.736           48    34299.668     0.676419           24            6            4
       12.757           48      156.663     0.060188           18           15            9
       12.757           48     3943.698     0.739427           19           13           10
       12.757           48    10074.289     0.481447           22           11            5
       12.757           48     1050.248     0.913322           23           10            1
       12.757           48    14211.491     0.658643           25            2            1
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       12.777           48    81153.352     0.580444           22           12            2
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       12.797           48     5481.227     0.572190           21           12            7
       12.797           48    18053.295     0.572190           24            7            3
       12.797           24        0.000     0.589848           25            3            0
       12.837           48     7405.788     0.689516           18           17            5
       12.837           48     2624.350     0.395211           19           14            9
       12.837           48     2138.960     0.801308           21           14            1
       12.837           48       10.241     1.610380           23           10            3
       12.837           48      475.319     1.107143           25            3            2
       12.857           24   400540.719     0.601597           24            8            0
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       12.878           48        0.125     0.568303           19           16            5
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       12.878           48      626.749     0.568173           25            4            1
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       12.898           48     5026.329     0.567173           20           12           10
       12.898           48     1582.216     0.567173           22           12            4
       12.898           48    10010.276     0.567173           24            8            2
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       12.918           48      222.695     0.098690           21           13            6
       12.918           48     6281.894     0.448796           21           14            3
       12.918           24      124.054     0.027292           22            9            9
       12.918           48     7534.736     0.458458           23            9            6
       12.938           24     6316.977     0.786949           16           14           14
       12.938           12    29334.926     0.663537           18           18            0
       12.938           48     1147.344     1.143397           22           10            8
       12.938           24     3723.319     0.331233           24            6            6
       12.958           48    19312.793     0.564184           16           15           13
       12.958           48     1304.676     0.564185           19           15            8
       12.958           24        0.000     0.629484           19           17            0
       12.958           48     7762.704     0.564184           20           13            9
       12.958           48        0.036     0.564203           20           15            5
       12.958           24        0.000     0.552595           23           11            0
       12.958           48     1174.496     0.564185           24            7            5
       12.958           48     1864.236     0.564185           25            4            3
       12.958           24        0.000     0.610466           25            5            0
       12.977           24        0.000     1.007893           18           18            2
       12.997           48     1257.012     0.317586           17           14           13
       12.997           48      803.021     0.965953           19           17            2
       12.997           48     3526.509     0.407812           22           11            7
       12.997           48    33105.316     0.617943           22           13            1
       12.997           48     3190.903     0.400563           23           10            5
       12.997           48     2609.250     0.385052           23           11            2
       12.997           48      628.391     0.236561           25            5            2
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       13.017           24    20781.746     0.576011           20           16            0
       13.017           48    89788.805     0.568307           24            8            4
       13.037           48    46834.953     0.560224           17           15           12
       13.037           48     4458.039     0.560224           24            9            1
       13.057           48    64854.797     0.633972           20           14            8
       13.057           48     1893.262     1.063184           20           16            2
       13.077           24    11205.765     0.468121           18           13           13
       13.077           48     2285.663     0.369342           18           17            7
       13.077           48      339.441     0.148501           21           11           10
       13.077           48     8367.582     0.454671           21           14            5
       13.077           48     7108.424     0.446360           22           13            3
       13.077           48    21281.016     0.492060           25            6            1
       13.096           48    68508.367     0.565478           18           14           12
       13.096           24   155737.828     0.562708           18           18            4
       13.096           48   103275.125     0.563951           22           12            6
       13.116           48       11.861     0.556303           17           16           11
       13.116           48        9.261     0.556294           19           16            7
       13.116           48      858.044     0.556291           19           17            4
       13.116           48     3173.471     0.556291           21           12            9
       13.116           24        0.000     0.612472           21           15            0
       13.116           48     3159.007     0.556291           23           11            4
       13.116           48    11758.186     0.556291           24            9            3
       13.116           48      817.126     0.556292           25            5            4
       13.155           48     2785.415     0.760410           18           15           11
       13.155           48    12620.544     0.468744           21           15            2
       13.155           48     9819.387     0.660046           25            6            3
       13.175           48    16619.480     0.433205           20           16            4
       13.195           48     1551.486     0.552387           19           13           12
       13.195           48     2451.736     0.552386           20           15            7
       13.195           48     8249.820     0.552386           21           13            8
       13.195           48     4248.809     0.552386           23            9            8
       13.195           48    21355.518     0.552386           23           12            1
       13.195           24        0.000     0.511862           24            7            7
       13.195           24        0.000     0.532794           25            7            0
       13.214           48       45.962     0.551413           24            8            6
       13.214           24     1375.366     0.551414           24           10            0
       13.214            6        0.000     0.581809           26            0            0
       13.234           24      125.795     1.815142           17           17           10
       13.234           48     3624.754     0.730497           19           14           11
       13.234           48    20871.211     0.622388           22           13            5
       13.234           48       16.691     0.846322           23           10            7
       13.234           48     1982.095     0.799991           25            7            2
       13.234           24     4838.143     0.704812           26            1            1
       13.253           48     6534.444     0.364097           18           16           10
       13.253           24     2222.547     0.955805           22           14            0
       13.253           48    24731.307     0.449439           24           10            2
       13.253           24     3270.319     0.298545           26            2            0
       13.273           48     7338.060     0.548509           21           15            4
       13.273           48     4058.442     0.548509           23           12            3
       13.273           48    14392.250     0.548509           24            9            5
       13.292           24        0.000     0.517475           18           18            6
       13.292           24        0.000     0.554471           22           10           10
       13.292           48     5628.166     0.547544           22           14            2
       13.292           24        0.000     0.523200           26            2            2
       13.311           48      727.746     0.986569           19           15           10
       13.311           48     5154.896     0.696772           19           17            6
       13.311           48     1101.667     0.894374           19           18            1
       13.311           48       81.138     2.249579           21           14            7
       13.311           48     2995.469     0.747331           22           11            9
       13.311           48     1254.767     0.869951           23           11            6
       13.311           48     2509.770     0.767480           25            6            5
       13.311           48     2730.918     0.757605           26            3            1
       13.331           24    43466.543     0.728675           20           12           12
       13.350           48      216.962     0.544659           20           13           11
       13.350           48     1647.968     0.544658           20           17            1
       13.350           48     4276.428     0.544658           25            7            4
       13.350           48    15238.885     0.544658           25            8            1
       13.370           48    84474.062     0.610509           20           16            6
       13.370           48    74722.828     0.614865           22           12            8
       13.370           48    40800.441     0.641053           24           10            4
       13.370           24   179990.234     0.589052           26            4            0
       13.389           48      404.751     0.154578           18           17            9
       13.389           48     4652.005     0.403703           19           18            3
       13.389           24      391.049     1.179888           26            3            3
       13.408           48   232808.609     0.546398           20           14           10
       13.408           48    99927.586     0.548833           22           14            4
       13.408           48   188579.734     0.546911           26            4            2
       13.427           48      641.491     0.540835           19           16            9
       13.427           48     3573.906     0.540835           20           17            3
       13.427           48     1412.832     0.540835           21           16            1
       13.427           48     2392.580     0.540836           23           12            5
       13.427           24        0.000     0.583230           23           13            0
       13.427           48    13539.380     0.540835           24           11            1
       13.427           48     4325.955     0.540835           25            8            3
       13.466           48    24231.410     0.475178           21           15            6
       13.466           48     2542.877     0.355048           22           13            7
       13.466           48     9143.574     0.651304           23           13            2
       13.466           48    44289.496     0.491389           26            5            1
       13.485           24   386159.906     0.572714           24            8            8
       13.504           24        0.000     0.537275           16           15           15
       13.504           48       79.871     0.537040           20           15            9
       13.504           48    17695.494     0.537038           21           12           11
       13.504           48      895.248     0.537037           21           16            3
       13.504           48    12284.010     0.537038           24            9            7
       13.504           48     2309.103     0.537038           24           11            3
       13.504           24        0.000     0.591044           25            9            0
       13.523           24        0.000     0.402816           16           16           14
       13.523           24        0.000     0.504490           26            4            4
       13.542           48     9775.623     0.436148           17           15           14
       13.542           48     7637.786     0.659352           19           18            5
       13.542           48      804.636     0.959318           21           13           10
       13.542           48     3708.660     0.379537           22           15            1
       13.542           48     7600.334     0.423640           23           10            9
       13.542           48      924.706     0.926972           25            7            6
       13.542           48     1905.093     0.325385           25            9            2
       13.542           48     2232.918     0.339564           26            5            3
       13.561           24    21222.117     0.656080           18           18            8
       13.561           48     7232.998     0.354522           24           10            6
       13.561           24     9536.754     0.720598           26            6            0
       13.580           48        7.376     0.533264           17           16           13
       13.580           48     8833.213     0.533268           19           17            8
       13.580           48      507.977     0.533268           20           17            5
       13.580           48     4764.306     0.533268           23           11            8
       13.580           48    16286.252     0.533268           23           13            4
       13.580           48    13357.467     0.533268           25            8            5
       13.599           24        0.000     0.552398           18           14           14
       13.599           48      240.404     0.532327           22           14            6
       13.599           48      142.940     0.532329           26            6            2
       13.618           48     1512.714     0.298800           18           15           13
       13.618           48    13081.259     0.444836           21           14            9
       13.618           48     5860.847     0.404917           22           15            3
       13.637           48    68102.938     0.539222           20           16            8
       13.637           24   161144.547     0.536148           24           12            0
       13.656           24        0.000     0.567319           17           17           12
       13.656           12        0.000     0.641853           19           19            0
       13.656           48     1567.160     0.529524           21           16            5
       13.656           48     1346.462     0.529525           23           12            7
       13.656           48    21105.100     0.529525           24           11            5
       13.656           48    24573.625     0.529525           25            9            4
       13.675           48    55987.738     0.613047           18           16           12
       13.675           24   294443.688     0.564651           20           18            0
       13.675           48    83364.617     0.597342           24           12            2
       13.694           48    21622.609     0.459374           19           14           13
       13.694           24      833.602     0.229171           19           19            2
       13.694           24    41057.730     0.580182           22           11           11
       13.694           48      258.246     0.079186           23           14            1
       13.694           48    12107.555     0.626306           25           10            1
       13.694           24     5123.758     0.392501           26            5            5
       13.694           48     1369.571     0.284268           26            7            1
       13.713           48   123013.125     0.533304           20           18            2
       13.713           48    71978.680     0.535331           22           12           10
       13.713           48    60597.105     0.536107           26            6            4
       13.732           48    36370.348     0.525808           19           15           12
       13.732           48     6984.553     0.525808           21           15            8
       13.732           24        0.000     0.556326           21           17            0
       13.732           24        0.000     0.520802           27            1            0
       13.769           48      805.905     0.956158           18           17           11
       13.769           48     3654.744     0.365521           19           18            7
       13.769           48    11134.515     0.429707           21           17            2
       13.769           48      514.928     1.084913           22           13            9
       13.769           48     1388.901     0.841474           22           15            5
       13.769           48     5090.758     0.680468           23           13            6
       13.769           48      118.760     1.919536           23           14            3
       13.769           48     2065.000     0.778836           25           10            3
       13.769           48     1673.389     0.810194           26            7            3
       13.769           48     1752.430     0.304277           27            2            1
       13.788           48      115.481     0.140374           24           12            4
       13.807           48    13001.454     0.522117           19           16           11
       13.807           24        0.000     0.550671           19           19            4
       13.807           24        0.000     0.644168           20           13           13
       13.807           48     3757.070     0.522116           20           17            7
       13.807           24        0.000     0.619965           24            9            9
       13.807           48      166.534     0.522118           25            8            7
       13.807           24        0.000     0.642318           27            3            0
       13.825           48      432.177     0.521196           20           14           12
       13.825           48    12337.985     0.521198           20           18            4
       13.825           24     6312.746     0.521198           22           16            0
       13.825           48     1634.139     0.521198           24           10            8
       13.825           24     6345.703     0.521198           26            8            0
       13.844           48     1706.373     0.805092           25            9            6
       13.844           48     3221.206     0.721440           27            3            2
       13.863           48     3274.244     0.263069           22           14            8
       13.863           48     3664.048     0.274854           22           16            2
       13.863           48     4512.130     0.805788           26            8            2
       13.881           48      202.873     0.518453           20           15           11
       13.881           48       53.521     0.518447           21           16            7
       13.881           48      164.154     0.518448           21           17            4
       13.881           48     4790.123     0.518451           24           11            7
       13.881           48      143.928     0.518449           24           13            1
       13.881           24        0.000     0.551518           25           11            0
       13.881           48     5639.001     0.518451           27            4            1
       13.900           24        0.000     0.480472           18           18           10
       13.900           24        0.000     0.536103           26            6            6
       13.919           48     4715.988     0.374636           19           17           10
       13.919           48     1152.720     0.252972           23           11           10
       13.919           48    14412.105     0.608090           23           14            5
       13.919           48     8711.256     0.409941           25           10            5
       13.919           48    12031.894     0.425067           25           11            2
       13.919           48      997.063     0.904037           26            7            5
       13.956           48     1712.422     0.514812           21           13           12
       13.956           48       51.106     0.514808           23           12            9
       13.956           24        0.000     0.493669           23           15            0
       13.956           48     3151.326     0.514811           24           13            3
       13.956           48     4966.151     0.514812           27            4            3
       13.956           24        0.000     0.544797           27            5            0
       13.974           48   184851.469     0.560507           20           16           10
       13.974           48    70229.789     0.590530           22           16            4
       13.974           48   102809.844     0.576854           24           12            6
       13.974           48    77585.695     0.586684           26            8            4
       13.993           24    27149.818     0.579212           19           19            6
       13.993           48     2431.204     0.749978           21           14           11
       13.993           48    34488.859     0.457621           22           15            7
       13.993           48      364.326     0.108468           23           15            2
       13.993           48     1418.150     0.270548           26            9            1
       13.993           48     9578.805     0.410609           27            5            2
       14.011           48    46500.246     0.523157           20           18            6
       14.030           48        0.084     0.511293           20           19            1
       14.030           48     3199.971     0.511198           23           13            8
       14.030           48    13297.949     0.511198           25           11            4

-------------- next part --------------
# 0.600000 0.003500 0.050000 0.000100 # sample: packing radius height wall
# 1.472205 0.153000 0.100000 0.053205 3.000000 # PSD: radius height pitch gap pressure
  1889.494   133.139  19.677 # YIG powder: Vc sigma_abs sigma_inc
  1111 YIG
        0.719           12        0.000     0.998322            1            1            0
        1.016            6        0.000     0.996636            2            0            0
        1.245           24      203.580     0.984168            2            1            1
        1.438           12     3016.019     0.986776            2            2            0
        1.607           24        0.000     0.992151            3            1            0
        1.761            8        0.000     0.989722            2            2            2
        1.902           48     1506.029     0.978739            3            2            1
        2.033            6    98281.828     0.986199            4            0            0
        2.156           12        0.000     0.986071            3            3            0
        2.156           24        0.000     0.981520            4            1            1
        2.273           24    54691.691     0.986475            4            2            0
        2.384           24    36367.449     0.977947            3            3            2
        2.490           24    18260.684     0.979746            4            2            2
        2.592           48    13085.104     0.977365            4            3            1
        2.592           24        0.000     0.980939            5            1            0
        2.784           48     9884.264     0.981401            5            2            1
        2.875           12    11381.769     0.984795            4            4            0
        2.963           24        0.000     0.972488            4            3            3
        2.963           24        0.000     0.974189            5            3            0
        3.049           24        0.000     0.970052            4            4            2
        3.049            6        0.000     0.980046            6            0            0
        3.133           48     4738.101     0.980699            5            3            2
        3.133           24    26526.645     0.972831            6            1            1
        3.214           24    17280.061     0.952795            6            2            0
        3.294           48     1072.821     0.963691            5            4            1
        3.371           24        0.000     0.964791            6            2            2
        3.447           48     5640.986     0.945413            6            3            1
        3.521            8   108324.977     0.971225            4            4            4
        3.594           48      710.790     0.956927            5            4            3
        3.594           12        0.000     0.972702            5            5            0
        3.594           24        0.000     0.964389            7            1            0
        3.665           24   190097.016     0.960594            6            4            0
        3.735           24     8854.975     0.967531            5            5            2
        3.735           24     2605.230     0.928074            6            3            3
        3.735           48      136.468     0.844741            7            2            1
        3.803           48   127188.094     0.952464            6            4            2
        3.871           24        0.000     0.959452            7            3            0
        4.002           48       48.465     1.173685            6            5            1
        4.002           48    14212.914     0.934375            7            3            2
        4.066            6   244666.688     0.951433            8            0            0
        4.129           24        0.000     0.941082            5            5            4
        4.129           48     7215.575     0.943539            7            4            1
        4.129           24        0.000     0.937901            8            1            1
        4.191           24        0.000     0.946819            6            4            4
        4.191           24    17019.494     0.941878            8            2            0
        4.252           48     8083.322     0.921666            6            5            3
        4.313           12      734.671     1.049026            6            6            0
        4.313           24    10628.211     0.910545            8            2            2
        4.372           48     7646.340     0.936915            7            4            3
        4.372           24        0.000     0.915093            7            5            0
        4.372           48      776.047     0.936915            8            3            1
        4.431           24        0.000     0.930654            6            6            2
        4.489           48     8357.111     0.913423            7            5            2
        4.546           24    99628.523     0.932912            8            4            0
        4.602           24        0.000     0.925655            8            3            3
        4.602           24        0.000     0.927404            9            1            0
        4.658           48    41391.684     0.946833            8            4            2
        4.713           24     6454.844     0.952557            6            5            5
        4.713           48    20689.980     0.912980            7            6            1
        4.713           48     1554.205     0.876190            9            2            1
        4.768           24    82241.906     0.926566            6            6            4
        4.822           48    21384.988     0.923807            7            5            4
        4.822           48    15318.223     0.923807            8            5            1
        4.822           24        0.000     0.925684            9            3            0
        4.928           48      504.394     0.824814            7            6            3
        4.928           48       19.874     1.482843            9            3            2
        4.980           24    16359.466     0.889442            8            4            4
        5.031           12        0.000     0.922682            7            7            0
        5.031           48    39592.711     0.917322            8            5            3
        5.031           48    25325.520     0.917322            9            4            1
        5.082           24      129.762     0.915708            8            6            0
        5.082            6        0.000     0.924715           10            0            0
        5.133           24     1579.174     0.975029            7            7            2
        5.133           24    20095.832     0.897369           10            1            1
        5.183           48      673.349     1.077036            8            6            2
        5.183           24    43752.160     0.932161           10            2            0
        5.233           48    10300.698     0.910883            9            4            3
        5.233           24        0.000     0.893915            9            5            0
        5.282            8        0.000     0.903652            6            6            6
        5.282           24        0.000     0.903433           10            2            2
        5.330           48    11530.723     0.931612            7            6            5
        5.330           48      131.671     0.698822            9            5            2
        5.330           48     1564.328     0.844278           10            3            1
        5.426           24        0.000     0.903811            7            7            4
        5.426           24        0.000     0.911782            8            5            5
        5.426           48     5560.977     0.904489            8            7            1
        5.474           48    43032.797     0.926892            8            6            4
        5.474           24   121046.172     0.917166           10            4            0
        5.521           48      869.710     0.995956            9            6            1
        5.521           24     1071.323     0.986376           10            3            3
        5.567           48   100115.828     0.901113           10            4            2
        5.614           48     1334.206     0.898139            8            7            3
        5.614           48     1100.267     0.898139            9            5            4
        5.614           24        0.000     0.894209           11            1            0
        5.705           48       44.953     0.516079            9            6            3
        5.705           48    11047.518     0.922668           10            5            1
        5.705           48     4519.932     0.938451           11            2            1
        5.750           12   231623.359     0.905655            8            8            0
        5.795           24        0.000     0.898561            9            7            0
        5.795           24        0.000     0.895735           11            3            0
        5.839           24        0.000     0.902606            8            8            2
        5.839           24        0.000     0.884242           10            4            4
        5.883           24    24914.727     0.869469            7            7            6
        5.883           48     7679.861     0.854214            9            7            2
        5.883           48      125.314     1.182243           10            5            3
        5.883           48     1178.122     0.802006           11            3            2
        5.927           24     7067.095     0.950199            8            6            6
        5.927           24    11585.631     0.936204           10            6            0
        5.970           48      462.440     0.885574            8            7            5
        5.970           48     5778.562     0.885574           11            4            1
        6.014           48    22267.492     0.884016           10            6            2
        6.056           48      486.486     1.034189            9            6            5
        6.099           24    72231.336     0.882867            8            8            4
        6.099            6    19129.297     0.884716           12            0            0
        6.141           48       72.866     0.879357            9            7            4
        6.141           48    27934.947     0.879357            9            8            1
        6.141           48     5137.507     0.879357           11            4            3
        6.141           24        0.000     0.883748           11            5            0
        6.141           24        0.000     0.887918           12            1            1
        6.183           24    66256.578     0.901881           12            2            0
        6.225           24     1145.936     0.779438           10            5            5
        6.225           48     2368.012     0.946966           10            7            1
        6.225           48        2.107     0.093289           11            5            2
        6.266           48    84037.055     0.876638           10            6            4
        6.266           24   134249.734     0.876239           12            2            2
        6.307           48     1321.134     0.873184            9            8            3
        6.307           48    23028.475     0.873184           12            3            1
        6.388           48      378.576     0.698084           10            7            3
        6.388           48     1202.565     0.771261           11            6            1
        6.429           24     4163.282     0.777967           12            4            0
        6.469           24        0.000     0.847652            8            7            7
        6.469           12        0.000     0.913683            9            9            0
        6.469           48     1046.849     0.867055           11            5            4
        6.469           24        0.000     0.732765           12            3            3
        6.509           24        0.000     0.861072            8            8            6
        6.509           24    10020.346     0.865529           10            8            0
        6.509           48      100.722     0.865529           12            4            2
        6.548           48     5719.824     0.913443            9            7            6
        6.548           24    10481.625     0.900393            9            9            2
        6.548           48    34038.199     0.884106           11            6            3
        6.587           48     2212.532     0.734415           10            8            2
        6.627           48     8340.317     0.860968            9            8            5
        6.627           24        0.000     0.864604           11            7            0
        6.627           48     1144.634     0.860968           12            5            1
        6.627           24        0.000     0.866319           13            1            0
        6.665           24        0.000     0.861820           10            6            6
        6.704           48     4163.081     0.799453           10            7            5
        6.704           48     2879.308     0.931003           11            7            2
        6.704           48    18606.156     0.830018           13            2            1
        6.743           24    31417.455     0.935357           12            4            4
        6.781           24        0.000     0.851566            9            9            4
        6.781           48    19656.873     0.854924           12            5            3
        6.781           24        0.000     0.899097           13            3            0
        6.819           48   154874.438     0.872072           10            8            4
        6.819           24    45146.090     0.888126           12            6            0
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        6.856           48       51.244     1.500796           11            6            5
        6.856           48     1127.712     0.974933           13            3            2
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        6.931           48    34190.152     0.848923           11            7            4
        6.931           48     2164.648     0.848923           11            8            1
        6.931           48      524.398     0.848923           13            4            1
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        7.079           48       91.726     0.842964           11            8            3
        7.079           24        0.000     0.833867           12            5            5
        7.079           48      236.346     0.842964           12            7            1
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        7.079           24        0.000     0.818209           13            5            0
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        7.152           24    10563.778     0.798793           10            7            7
        7.152           48    29967.029     0.815409           13            5            2
        7.152           24      871.975     0.991503           14            1            1
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        7.188           12    61323.203     0.809452           10           10            0
        7.188           24    15699.059     0.781564           14            2            0
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        7.223           48    26204.113     0.837046           12            7            3
        7.259           24        0.000     0.837881           10           10            2
        7.259           24        0.000     0.829693           14            2            2
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        7.295           48     1751.051     0.731513           11            7            6
        7.295           48     1620.526     0.947878           11            9            2
        7.295           48     5809.077     0.776945           13            6            1
        7.295           48     3604.480     0.909587           14            3            1
        7.330           24    73445.188     0.835414           12            8            0
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        7.365           48     5873.266     0.831170           13            5            4
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        7.400           24    54682.270     0.865962           14            4            0
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        7.435           24     2714.380     0.742726           14            3            3
        7.470           24   165646.812     0.828709           10           10            4
        7.470           24    74290.812     0.829656           12            6            6
        7.470           48   151288.562     0.828798           14            4            2
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        7.504           48     5411.900     0.825336           12            7            5
        7.504           24        0.000     0.822316           13            7            0
        7.573           48     1254.346     0.694604           11           10            1
        7.573           48      148.693     0.481002           13            7            2
        7.573           48    30448.402     0.795615           14            5            1
        7.607           48     1966.262     1.010599           12            8            4
        7.640           24        0.000     0.827541            9            9            8
        7.640           48     6363.631     0.819542           12            9            1
        7.640           24        0.000     0.837935           15            1            0
        7.674           24        0.000     0.824846           10            8            8
        7.674           24        0.000     0.818697           14            4            4
        7.708           48     3849.914     0.896828           10            9            7
        7.708           48     1094.647     0.676433           11           10            3
        7.708           48       79.345     0.362349           13            6            5
        7.708           48       79.048     1.454426           14            5            3
        7.708           48     5521.893     0.883341           15            2            1
        7.741           24       74.444     0.141779           14            6            0
        7.775           48    15044.647     0.813789           11            8            7
        7.775           48    11309.317     0.813789           12            9            3
        7.775           48    14739.329     0.813789           13            7            4
        7.775           48     3247.167     0.813789           13            8            1
        7.775           24        0.000     0.828548           15            3            0
        7.808           24        0.000     0.844919           10           10            6
        7.808           48    11997.312     0.812357           14            6            2
        7.841           48    19856.273     0.775865           11            9            6
        7.841           48    13406.674     0.854643           15            3            2
        7.906           12        0.000     0.816166           11           11            0
        7.906           24        0.000     0.830149           12            7            7
        7.906           48     7061.392     0.808076           13            8            3
        7.906           48     2060.587     0.808076           15            4            1
        7.939           48    93269.773     0.837780           12            8            6
        7.939           24    47890.504     0.850255           12           10            0
        7.971           48     7796.717     0.748176           11           10            5
        7.971           24     7086.558     0.745438           11           11            2
        7.971           24     2328.366     0.702413           14            5            5
        7.971           48       19.962     0.066294           14            7            1
        8.004           48   112340.125     0.806478           12           10            2
        8.004           48    53296.637     0.807681           14            6            4
        8.036           48    14131.926     0.802403           12            9            5
        8.036           24        0.000     0.829866           13            9            0
        8.036           48      956.852     0.802403           15            4            3
        8.036           24        0.000     0.785195           15            5            0
        8.100           48      125.046     1.339667           13            7            6
        8.100           48     2835.213     0.703768           13            9            2
        8.100           48       10.602     0.000098           14            7            3
        8.100           48     1178.623     0.653589           15            5            2
        8.132            6   151833.891     0.825886           16            0            0
        8.163           24        0.000     0.795598           11           11            4
        8.163           48     1550.868     0.796771           13            8            5
        8.163           24        0.000     0.872871           16            1            1
        8.195           48      242.107     0.795369           12           10            4
        8.195           24    33236.344     0.795369           14            8            0
        8.195           24    34660.660     0.795369           16            2            0
        8.227           24    12606.899     0.842757           10            9            9
        8.227           48     2381.923     0.687250           15            6            1
        8.258           24      864.789     0.513735           10           10            8
        8.258           48     6570.184     0.908619           14            8            2
        8.258           24     6778.777     0.906760           16            2            2
        8.289           48      966.176     0.791177           11            9            8
        8.289           48    43581.391     0.791178           12           11            1
        8.289           48     7196.764     0.791178           13            9            4
        8.289           48    10670.142     0.791177           15            5            4
        8.289           48     3204.440     0.791177           16            3            1
        8.320           24        0.000     0.808097           14            6            6
        8.351           48      200.804     1.226601           11           10            7
        8.351           48     2200.392     0.910606           13           10            1
        8.351           48     1091.037     0.629967           14            7            5
        8.351           48     3256.225     0.888213           15            6            3
        8.382           24    93462.555     0.790193           12            8            8
        8.382           24    75682.148     0.790548           16            4            0
        8.413           48    11445.481     0.785624           12            9            7
        8.413           48      142.793     0.785624           12           11            3
        8.413           24        0.000     0.807413           15            7            0
        8.413           24        0.000     0.793343           16            3            3
        8.443           48    66963.406     0.824903           14            8            4
        8.443           48   152509.391     0.811070           16            4            2
        8.474           24      991.613     0.613598           11           11            6
        8.474           48     1375.104     0.637806           13           10            3
        8.474           48     3873.620     0.694648           14            9            1
        8.474           48     6604.764     0.853982           15            7            2
        8.504           48   105229.992     0.784568           12           10            6
        8.535           48    20650.426     0.780109           13            8            7
        8.535           48    11068.548     0.780109           16            5            1
        8.595           48     1777.985     0.920500           13            9            6
        8.595           48     9026.879     0.839398           14            9            3
        8.595           48     1867.975     0.649371           15            6            5
        8.625           12      440.601     0.382222           12           12            0
        8.625           24     4123.180     0.934647           16            4            4
        8.655           48     2586.402     0.774632           12           11            5
        8.655           24        0.000     0.773600           13           11            0
        8.655           48        3.233     0.774635           15            7            4
        8.655           48    53071.383     0.774632           15            8            1
        8.655           48     3789.377     0.774632           16            5            3
        8.655           24        0.000     0.795470           17            1            0
        8.685           24        0.000     0.771895           12           12            2
        8.685           24     3643.341     0.773269           16            6            0
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        8.744           24     2282.333     0.576950           14           10            0
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        8.803           48      454.897     0.767840           14           10            2
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        8.832           48     6171.375     0.845140           14            9            5
        8.832           48      590.266     1.034670           17            3            2
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        8.890           24        0.000     0.770600           11           11            8
        8.890           24        0.000     0.675269           12            9            9
        8.890           48     9594.028     0.763795           13           11            4
        8.890           24        0.000     0.801700           15            9            0
        8.890           24        0.000     0.763028           16            5            5
        8.890           48    11653.093     0.763795           16            7            1
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        8.919           48    41982.527     0.818643           12           10            8
        8.919           48    84537.617     0.801842           16            6            4
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        8.948           48     6684.949     0.687764           15            9            2
        8.977           48    31867.904     0.765981           14           10            4
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        9.006           48       58.134     0.758433           13            9            8
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        9.063           48      935.103     0.974633           14           11            1
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        9.148           24        0.000     0.725124           14            8            8
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        9.562           24        0.000     0.779491           16            7            7
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        9.829           48      285.456     1.197523           17            9            2
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        9.985           24        0.000     0.731896           19            5            0
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       10.037           48        0.061   333.109955           14           13            5
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       10.037           48    10274.168     0.639479           19            5            2
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       10.088           24        0.000     0.738399           15           13            0
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       10.114           24        0.000     0.757605           18            6            6
       10.139           48     7466.300     0.621679           14           11            9
       10.139           48      990.249     0.957920           15           13            2
       10.139           48     1190.770     0.934025           17           10            3
       10.139           48        9.645     0.329466           18            7            5
       10.139           48     8873.878     0.784734           19            6            1
       10.165           24   135888.438     0.706895           16           12            0
       10.165            6   200452.516     0.706227           20            0            0
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       10.190           48     3440.059     0.701881           19            5            4
       10.190           24        0.000     0.664889           20            1            1
       10.215           48   103570.594     0.744078           14           12            8
       10.215           48    78204.258     0.750741           16           12            2
       10.215           48   108975.664     0.742971           18            8            4
       10.215           24   200123.938     0.731759           20            2            0
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       10.241           48      821.729     0.463152           17            9            6
       10.241           48      183.235     0.256509           18            9            1
       10.241           48       11.070     4.744914           19            6            3
       10.266           24    85986.914     0.703017           14           14            4
       10.266           24   176294.906     0.701557           20            2            2
       10.291           48     1421.877     0.696954           15           11            8
       10.291           48    10078.014     0.696954           15           13            4
       10.291           24        0.000     0.705679           17           11            0
       10.291           24        0.000     0.727756           19            7            0
       10.291           48        7.288     0.696954           20            3            1
       10.341           48      211.520     1.312292           14           13            7
       10.341           48     1385.313     0.912704           17           10            5
       10.341           48    16359.064     0.636597           17           11            2
       10.341           48      490.017     0.394712           18            9            3
       10.341           48     6772.580     0.789503           19            7            2
       10.366           48     1908.914     0.434801           16           12            4
       10.366           24    23541.840     0.613565           20            4            0
       10.391           48     5924.918     0.692061           15           12            7
       10.391           24        0.000     0.799210           16            9            9
       10.391           24        0.000     0.729334           20            3            3
       10.416           48     6394.384     0.690844           16           10            8
       10.416           48     3046.540     0.690844           20            4            2
       10.440           48     2461.563     0.543780           15           14            1
       10.440           24      135.264     1.506200           18            7            7
       10.440           48    19656.266     0.636037           19            6            5
       10.465           48    22722.738     0.606361           18            8            6
       10.465           24    17729.400     0.595911           18           10            0
       10.490           48     5276.253     0.687204           16           11            7
       10.490           48      448.920     0.687203           16           13            1
       10.490           48     8295.166     0.687203           17           11            4
       10.490           48      139.147     0.687203           19            7            4
       10.490           48        0.328     0.687215           19            8            1
       10.490           48     3527.839     0.687203           20            5            1
       10.514           24        0.000     0.727619           14           14            6
       10.514           48    48499.012     0.685994           18           10            2
       10.539           48      647.314     0.413689           15           13            6
       10.539           48    26527.465     0.637960           15           14            3
       10.539           48      487.215     0.378284           18            9            5
       10.563            8    52768.902     0.807684           12           12           12
       10.563           24    92219.422     0.776506           20            4            4
       10.588           48     5757.705     0.682379           13           12           11
       10.588           48     9340.360     0.682379           16           13            3
       10.588           48      710.295     0.682379           17            9            8
       10.588           48    10436.022     0.682379           17           12            1
       10.588           48    27884.703     0.682379           19            8            3
       10.588           48        5.528     0.682372           20            5            3
       10.612           48    62078.328     0.740588           16           12            6
       10.612           24     2835.733     0.980520           20            6            0
       10.637           24      336.916     1.175382           13           13           10
       10.637           24    33559.977     0.637768           14           11           11
       10.637           48      930.464     0.961942           17           10            7
       10.661           48    98878.328     0.683607           14           12           10
       10.661           48    42282.145     0.686166           18           10            4
       10.661           48    68886.531     0.684564           20            6            2
       10.685           48     1498.741     0.677589           17           12            3
       10.685           24        0.000     0.698189           19            9            0
       10.685           24        0.000     0.703940           21            1            0
       10.733           48     2054.250     0.511190           14           13            9
       10.733           48    13512.246     0.608545           15           11           10
       10.733           48      874.002     0.433063           15           14            5
       10.733           48     8341.328     0.765061           17           11            6
       10.733           48     3496.692     0.547453           18           11            1
       10.733           48     5957.996     0.576137           19            7            6
       10.733           48     1422.699     0.480880           19            9            2
       10.733           48       29.973     2.908144           21            2            1
       10.781           48     1753.692     0.672832           15           12            9
       10.781           12        0.000     0.664564           15           15            0
       10.781           48     1753.916     0.672832           16           13            5
       10.781           48       40.492     0.672836           19            8            5
       10.781           24        0.000     0.690230           20            5            5
       10.781           48     3651.796     0.672833           20            7            1
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       10.805           24        0.000     0.643831           18            8            8
       10.805           48     9669.600     0.671649           20            6            4
       10.829           24    13108.416     0.602064           15           15            2
       10.829           48        7.145     1.037184           18            9            7
       10.829           48     5454.835     0.565999           18           11            3
       10.829           48    11229.632     0.748505           21            3            2
       10.853           24    15315.414     0.565674           14           14            8
       10.853           24    22509.879     0.761307           16           10           10
       10.853           48     3599.667     0.465110           16           14            2
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       10.877           48     6143.480     0.668110           16           11            9
       10.877           48     6768.690     0.668109           17           12            5
       10.877           24        0.000     0.688241           17           13            0
       10.877           48    21970.449     0.668109           19            9            4
       10.877           48     6369.703     0.668110           20            7            3
       10.877           48     1052.865     0.668110           21            4            1
       10.900           48     3017.939     0.666934           18           10            6
       10.924           48    19252.697     0.725662           17           13            2
       10.924           48    25930.057     0.616213           19           10            1
       10.948           48    84530.609     0.670057           16           12            8
       10.948           24    97406.680     0.669681           20            8            0
       10.971           24        0.000     0.685600           15           15            4
       10.971           48    10599.709     0.663419           21            4            3
       10.971           24        0.000     0.643299           21            5            0
       10.995           48   100173.562     0.711064           16           14            4
       10.995           24   166767.672     0.699932           18           12            0
       10.995           48   159852.547     0.700750           20            8            2
       11.018           48     1658.682     0.878372           15           14            7
       11.018           48    17370.697     0.600177           17           10            9
       11.018           48      597.529     0.367525           18           11            5
       11.018           48      997.503     0.426396           19           10            3
       11.018           48     3084.364     0.521335           21            5            2
       11.042           48   106769.031     0.664861           18           12            2
       11.042           24   137048.594     0.664281           20            6            6
       11.065           48     2199.089     0.658762           16           13            7
       11.065           48    22348.607     0.658762           17           11            8
       11.065           48     5517.560     0.658762           17           13            4
       11.065           48     2181.360     0.658762           19            8            7
       11.065           48      792.531     0.658762           20            7            5
       11.112           48       94.408     1.790153           19            9            6
       11.112           48     8604.981     0.749077           21            6            1
       11.135           48    12669.628     0.783483           20            8            4
       11.158           24        0.000     0.646298           13           13           12
       11.158           48     9421.717     0.654138           16           15            1
       11.158           48      210.036     0.654139           17           12            7
       11.158           24        0.000     0.710653           19           11            0
       11.158           48       92.088     0.654137           20            9            1
       11.158           48     2810.931     0.654138           21            5            4
       11.181           24        0.000     0.727377           14           12           12
       11.181           48     5305.505     0.652987           18           12            4
       11.181            6        0.000     0.654133           22            0            0
       11.204           48    15691.037     0.720583           14           13           11
       11.204           24    33526.344     0.606793           15           15            6
       11.204           48     3536.515     0.800657           17           14            1
       11.204           24      287.097     0.250511           18            9            9
       11.204           48     7806.454     0.750322           19           10            5
       11.204           48      812.864     0.390627           19           11            2
       11.204           48     8561.631     0.745729           21            6            3
       11.204           24    20528.598     0.594559           22            1            1
       11.227           48       14.069     2.231752           16           14            6
       11.227           48     3712.752     0.899219           18           10            8
       11.227           24      759.892     1.253699           22            2            0
       11.250           48      487.995     0.649546           15           12           11
       11.250           48     2527.021     0.649546           16           15            3
       11.250           48     4456.323     0.649545           20            9            3
       11.250           24        0.000     0.652303           21            7            0
       11.273           24        0.000     0.789600           14           14           10
       11.273           24        0.000     0.653409           22            2            2
       11.296           48      706.681     0.367562           15           13           10
       11.296           48      297.195     0.248811           17           13            6
       11.296           48     7711.250     0.554293           17           14            3
       11.296           48     2570.974     0.490818           18           11            7
       11.296           48     8067.584     0.745120           18           13            1
       11.296           48    22961.691     0.704436           21            7            2
       11.296           48       87.333     0.057870           22            3            1
       11.342           24        0.000     0.685507           16           11           11
       11.342           48      332.649     0.644986           19           11            4
       11.342           24        0.000     0.746241           20            7            7
       11.364           48   159977.438     0.683996           16           12           10
       11.364           48   130867.500     0.688308           20            8            6
       11.364           24    72803.609     0.703794           20           10            0
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       11.387           48       14.392     4.882132           18           13            3
       11.387           48     1769.587     0.455264           21            6            5
       11.387           24    51470.301     0.681020           22            3            3
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       11.432           48    31403.549     0.640459           19            9            8
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       11.432           48     2748.602     0.640458           20            9            5
       11.432           48      346.130     0.640457           21            7            4
       11.432           48     8339.304     0.640458           21            8            1
       11.478           48     5003.653     0.521834           17           11           10
       11.478           48     3454.537     0.793780           17           14            5
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       11.522           48     6706.062     0.635963           21            8            3
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       11.545           24        0.000     0.657954           22            4            4
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       11.567           48     8971.104     0.729207           18           13            5
       11.567           48     7212.025     0.535136           19           11            6
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       11.612           24        0.000     0.667525           21            9            0
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       11.745           48    21234.656     0.565384           17           14            7
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       11.745           48    14864.012     0.554119           23            2            1
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       11.766           48   163276.672     0.628214           18           14            4
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       11.788           48    12175.204     0.622663           21            9            4
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       11.876           48     4312.363     0.618292           20           11            5
       11.876           48       68.349     0.618293           23            4            1
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       11.919           48     6327.436     0.507762           17           15            6
       11.919           48     4055.922     0.482407           18           15            1
       11.919           48      242.952     0.172778           21           10            3
       11.941           48     7888.565     0.458459           16           14           10
       11.941           48      109.173     2.873094           22            8            2
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       11.962           48    16083.902     0.613952           17           16            3
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       11.962           48        1.472     0.613933           21            8            7
       11.962           48    37939.918     0.613952           23            4            3
       11.962           24        0.000     0.616921           23            5            0
       11.984           48     1296.799     0.612872           18           14            6
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       12.006           48       82.405     2.026851           17           13           10
       12.006           48    18215.365     0.546157           18           15            3
       12.006           48     9411.382     0.709300           19           14            1
       12.006           48     2181.693     0.822372           21            9            6
       12.006           48      335.092     1.210647           22            7            5
       12.006           48     8659.716     0.517815           23            5            2
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       12.048           24        0.000     0.614455           20            9            9
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       12.070           48   105682.531     0.661900           22            8            4
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       12.091           24      972.384     0.937657           18           11           11
       12.091           48     1994.939     0.830481           19           13            6
       12.091           48        0.028  1184.492188           19           14            3
       12.091           48     3860.352     0.764279           21           10            5
       12.091           48     3519.251     0.462570           21           11            2
       12.091           48      775.554     0.981970           22            9            1
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       12.134           48     3683.249     0.605362           17           16            5
       12.134           48     3521.664     0.605362           20           11            7
       12.134           48      124.058     0.605363           20           13            1
       12.134           48     3462.126     0.605362           23            5            4
       12.176           48       55.890     0.000408           18           13            9
       12.176           48       97.423     1.905106           18           15            5
       12.176           48    14498.582     0.528827           22            9            3
       12.176           48     4836.832     0.477510           23            6            3
       12.198           24   146829.391     0.652999           16           16            8
       12.198            6    48972.145     0.691485           24            0            0
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       12.219           48     2019.349     0.601113           21           11            4
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       12.261           24    23870.430     0.540168           22            7            7
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       12.282           48     2399.438     0.325265           18           16            2
       12.282           48     8974.643     0.446666           22            8            6
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       12.303           48    16475.064     0.596893           21            9            8
       12.303           48    21749.035     0.596893           21           12            1
       12.303           48        0.566     0.596886           24            3            1
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       12.324           48    12293.235     0.595843           22           10            2
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       12.345           48     1708.446     0.389242           19           15            2
       12.345           48      516.791     1.079764           21           10            7
       12.345           48    11336.400     0.509842           22            9            5
       12.345           48    18111.604     0.527044           23            6            5
       12.366           24    58389.941     0.601851           24            4            0
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       12.387           24        0.000     0.735260           16           13           13
       12.387           48    12095.004     0.592703           17           16            7
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       12.387           48     1167.612     0.592703           20           13            5
       12.387           48      486.571     0.592703           21           12            3
       12.387           48      968.762     0.592702           23            7            4
       12.387           48     2560.149     0.592703           23            8            1
       12.387           24        0.000     0.590848           24            3            3
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       12.470           48    10761.667     0.588542           17           13           12
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       12.470           48    17676.646     0.588542           24            5            1
       12.511           48      236.687     0.130661           17           14           11
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       12.511           48    15084.020     0.511461           22           11            1
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       12.532           24     2797.412     0.326392           24            4            4
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       12.552           48     1401.835     0.584411           24            5            3
       12.573           24        0.000     0.628182           16           16           10
       12.573           24        0.000     0.574667           18           12           12
       12.573           48       27.689     0.583384           20           14            4
       12.573           24        0.000     0.593523           22            8            8
       12.573           24      974.674     0.583382           24            6            0
       12.594           48     7713.880     0.696704           17           15           10
       12.594           24      625.189     0.261879           17           17            6
       12.594           48      342.001     0.179135           18           13           11
       12.594           48     2097.192     0.810675           18           17            1
       12.594           48      486.338     1.098598           21           13            2
       12.594           48    19185.775     0.653674           22            9            7
       12.594           48      257.410     0.137906           22           11            3
       12.594           48    21796.854     0.649147           23            7            6
       12.594           48     2041.253     0.814043           23            9            2
       12.614           48    42259.598     0.660673           18           16            6
       12.614           48     1627.606     1.038560           24            6            2
       12.635           48        9.570     0.580310           19           16            1
       12.635           48     4582.844     0.580308           20           13            7
       12.635           48      424.410     0.580309           23            8            5
       12.655           48    31903.266     0.579287           18           14           10
       12.655           48     5253.120     0.579288           22           10            6
       12.675           48     2611.902     0.404740           18           17            3
       12.675           48    13236.974     0.497375           19           15            6
       12.675           48     1066.550     0.911786           21           10            9
       12.716           48     6204.871     0.576235           17           16            9
       12.716           48     6512.263     0.576235           19           12           11
       12.716           48     7935.641     0.576235           19           16            3
       12.716           48     1384.119     0.576235           20           15            1
       12.716           48     6295.197     0.576235           21           11            8
       12.716           48    24718.215     0.576235           21           13            4
       12.716           48     5930.177     0.576235           23            9            4
       12.716           24        0.000     0.586224           24            5            5
       12.716           48    14408.281     0.576235           24            7            1
       12.716           24        0.000     0.599632           25            1            0
       12.736           24   120591.719     0.628172           22           12            0
       12.736           48    34299.668     0.676419           24            6            4
       12.757           48      156.663     0.060188           18           15            9
       12.757           48     3943.698     0.739427           19           13           10
       12.757           48    10074.289     0.481447           22           11            5
       12.757           48     1050.248     0.913322           23           10            1
       12.757           48    14211.491     0.658643           25            2            1
       12.777           48   118851.406     0.579183           20           14            6
       12.777           48    81153.352     0.580444           22           12            2
       12.797           48     1636.235     0.572190           20           15            3
       12.797           48     5481.227     0.572190           21           12            7
       12.797           48    18053.295     0.572190           24            7            3
       12.797           24        0.000     0.589848           25            3            0
       12.837           48     7405.788     0.689516           18           17            5
       12.837           48     2624.350     0.395211           19           14            9
       12.837           48     2138.960     0.801308           21           14            1
       12.837           48       10.241     1.610380           23           10            3
       12.837           48      475.319     1.107143           25            3            2
       12.857           24   400540.719     0.601597           24            8            0
       12.878           24        0.000     0.594411           17           17            8
       12.878           48        0.125     0.568303           19           16            5
       12.878           24        0.000     0.668721           20           11           11
       12.878           48     9156.891     0.568173           23            8            7
       12.878           48      626.749     0.568173           25            4            1
       12.898           48      752.168     0.567174           18           16            8
       12.898           48     5026.329     0.567173           20           12           10
       12.898           48     1582.216     0.567173           22           12            4
       12.898           48    10010.276     0.567173           24            8            2
       12.918           24      201.271     1.472532           15           15           14
       12.918           48      222.695     0.098690           21           13            6
       12.918           48     6281.894     0.448796           21           14            3
       12.918           24      124.054     0.027292           22            9            9
       12.918           48     7534.736     0.458458           23            9            6
       12.938           24     6316.977     0.786949           16           14           14
       12.938           12    29334.926     0.663537           18           18            0
       12.938           48     1147.344     1.143397           22           10            8
       12.938           24     3723.319     0.331233           24            6            6
       12.958           48    19312.793     0.564184           16           15           13
       12.958           48     1304.676     0.564185           19           15            8
       12.958           24        0.000     0.629484           19           17            0
       12.958           48     7762.704     0.564184           20           13            9
       12.958           48        0.036     0.564203           20           15            5
       12.958           24        0.000     0.552595           23           11            0
       12.958           48     1174.496     0.564185           24            7            5
       12.958           48     1864.236     0.564185           25            4            3
       12.958           24        0.000     0.610466           25            5            0
       12.977           24        0.000     1.007893           18           18            2
       12.997           48     1257.012     0.317586           17           14           13
       12.997           48      803.021     0.965953           19           17            2
       12.997           48     3526.509     0.407812           22           11            7
       12.997           48    33105.316     0.617943           22           13            1
       12.997           48     3190.903     0.400563           23           10            5
       12.997           48     2609.250     0.385052           23           11            2
       12.997           48      628.391     0.236561           25            5            2
       13.017           24    57828.707     0.570060           16           16           12
       13.017           24    20781.746     0.576011           20           16            0
       13.017           48    89788.805     0.568307           24            8            4
       13.037           48    46834.953     0.560224           17           15           12
       13.037           48     4458.039     0.560224           24            9            1
       13.057           48    64854.797     0.633972           20           14            8
       13.057           48     1893.262     1.063184           20           16            2
       13.077           24    11205.765     0.468121           18           13           13
       13.077           48     2285.663     0.369342           18           17            7
       13.077           48      339.441     0.148501           21           11           10
       13.077           48     8367.582     0.454671           21           14            5
       13.077           48     7108.424     0.446360           22           13            3
       13.077           48    21281.016     0.492060           25            6            1
       13.096           48    68508.367     0.565478           18           14           12
       13.096           24   155737.828     0.562708           18           18            4
       13.096           48   103275.125     0.563951           22           12            6
       13.116           48       11.861     0.556303           17           16           11
       13.116           48        9.261     0.556294           19           16            7
       13.116           48      858.044     0.556291           19           17            4
       13.116           48     3173.471     0.556291           21           12            9
       13.116           24        0.000     0.612472           21           15            0
       13.116           48     3159.007     0.556291           23           11            4
       13.116           48    11758.186     0.556291           24            9            3
       13.116           48      817.126     0.556292           25            5            4
       13.155           48     2785.415     0.760410           18           15           11
       13.155           48    12620.544     0.468744           21           15            2
       13.155           48     9819.387     0.660046           25            6            3
       13.175           48    16619.480     0.433205           20           16            4
       13.195           48     1551.486     0.552387           19           13           12
       13.195           48     2451.736     0.552386           20           15            7
       13.195           48     8249.820     0.552386           21           13            8
       13.195           48     4248.809     0.552386           23            9            8
       13.195           48    21355.518     0.552386           23           12            1
       13.195           24        0.000     0.511862           24            7            7
       13.195           24        0.000     0.532794           25            7            0
       13.214           48       45.962     0.551413           24            8            6
       13.214           24     1375.366     0.551414           24           10            0
       13.214            6        0.000     0.581809           26            0            0
       13.234           24      125.795     1.815142           17           17           10
       13.234           48     3624.754     0.730497           19           14           11
       13.234           48    20871.211     0.622388           22           13            5
       13.234           48       16.691     0.846322           23           10            7
       13.234           48     1982.095     0.799991           25            7            2
       13.234           24     4838.143     0.704812           26            1            1
       13.253           48     6534.444     0.364097           18           16           10
       13.253           24     2222.547     0.955805           22           14            0
       13.253           48    24731.307     0.449439           24           10            2
       13.253           24     3270.319     0.298545           26            2            0
       13.273           48     7338.060     0.548509           21           15            4
       13.273           48     4058.442     0.548509           23           12            3
       13.273           48    14392.250     0.548509           24            9            5
       13.292           24        0.000     0.517475           18           18            6
       13.292           24        0.000     0.554471           22           10           10
       13.292           48     5628.166     0.547544           22           14            2
       13.292           24        0.000     0.523200           26            2            2
       13.311           48      727.746     0.986569           19           15           10
       13.311           48     5154.896     0.696772           19           17            6
       13.311           48     1101.667     0.894374           19           18            1
       13.311           48       81.138     2.249579           21           14            7
       13.311           48     2995.469     0.747331           22           11            9
       13.311           48     1254.767     0.869951           23           11            6
       13.311           48     2509.770     0.767480           25            6            5
       13.311           48     2730.918     0.757605           26            3            1
       13.331           24    43466.543     0.728675           20           12           12
       13.350           48      216.962     0.544659           20           13           11
       13.350           48     1647.968     0.544658           20           17            1
       13.350           48     4276.428     0.544658           25            7            4
       13.350           48    15238.885     0.544658           25            8            1
       13.370           48    84474.062     0.610509           20           16            6
       13.370           48    74722.828     0.614865           22           12            8
       13.370           48    40800.441     0.641053           24           10            4
       13.370           24   179990.234     0.589052           26            4            0
       13.389           48      404.751     0.154578           18           17            9
       13.389           48     4652.005     0.403703           19           18            3
       13.389           24      391.049     1.179888           26            3            3
       13.408           48   232808.609     0.546398           20           14           10
       13.408           48    99927.586     0.548833           22           14            4
       13.408           48   188579.734     0.546911           26            4            2
       13.427           48      641.491     0.540835           19           16            9
       13.427           48     3573.906     0.540835           20           17            3
       13.427           48     1412.832     0.540835           21           16            1
       13.427           48     2392.580     0.540836           23           12            5
       13.427           24        0.000     0.583230           23           13            0
       13.427           48    13539.380     0.540835           24           11            1
       13.427           48     4325.955     0.540835           25            8            3
       13.466           48    24231.410     0.475178           21           15            6
       13.466           48     2542.877     0.355048           22           13            7
       13.466           48     9143.574     0.651304           23           13            2
       13.466           48    44289.496     0.491389           26            5            1
       13.485           24   386159.906     0.572714           24            8            8
       13.504           24        0.000     0.537275           16           15           15
       13.504           48       79.871     0.537040           20           15            9
       13.504           48    17695.494     0.537038           21           12           11
       13.504           48      895.248     0.537037           21           16            3
       13.504           48    12284.010     0.537038           24            9            7
       13.504           48     2309.103     0.537038           24           11            3
       13.504           24        0.000     0.591044           25            9            0
       13.523           24        0.000     0.402816           16           16           14
       13.523           24        0.000     0.504490           26            4            4
       13.542           48     9775.623     0.436148           17           15           14
       13.542           48     7637.786     0.659352           19           18            5
       13.542           48      804.636     0.959318           21           13           10
       13.542           48     3708.660     0.379537           22           15            1
       13.542           48     7600.334     0.423640           23           10            9
       13.542           48      924.706     0.926972           25            7            6
       13.542           48     1905.093     0.325385           25            9            2
       13.542           48     2232.918     0.339564           26            5            3
       13.561           24    21222.117     0.656080           18           18            8
       13.561           48     7232.998     0.354522           24           10            6
       13.561           24     9536.754     0.720598           26            6            0
       13.580           48        7.376     0.533264           17           16           13
       13.580           48     8833.213     0.533268           19           17            8
       13.580           48      507.977     0.533268           20           17            5
       13.580           48     4764.306     0.533268           23           11            8
       13.580           48    16286.252     0.533268           23           13            4
       13.580           48    13357.467     0.533268           25            8            5
       13.599           24        0.000     0.552398           18           14           14
       13.599           48      240.404     0.532327           22           14            6
       13.599           48      142.940     0.532329           26            6            2
       13.618           48     1512.714     0.298800           18           15           13
       13.618           48    13081.259     0.444836           21           14            9
       13.618           48     5860.847     0.404917           22           15            3
       13.637           48    68102.938     0.539222           20           16            8
       13.637           24   161144.547     0.536148           24           12            0
       13.656           24        0.000     0.567319           17           17           12
       13.656           12        0.000     0.641853           19           19            0
       13.656           48     1567.160     0.529524           21           16            5
       13.656           48     1346.462     0.529525           23           12            7
       13.656           48    21105.100     0.529525           24           11            5
       13.656           48    24573.625     0.529525           25            9            4
       13.675           48    55987.738     0.613047           18           16           12
       13.675           24   294443.688     0.564651           20           18            0
       13.675           48    83364.617     0.597342           24           12            2
       13.694           48    21622.609     0.459374           19           14           13
       13.694           24      833.602     0.229171           19           19            2
       13.694           24    41057.730     0.580182           22           11           11
       13.694           48      258.246     0.079186           23           14            1
       13.694           48    12107.555     0.626306           25           10            1
       13.694           24     5123.758     0.392501           26            5            5
       13.694           48     1369.571     0.284268           26            7            1
       13.713           48   123013.125     0.533304           20           18            2
       13.713           48    71978.680     0.535331           22           12           10
       13.713           48    60597.105     0.536107           26            6            4
       13.732           48    36370.348     0.525808           19           15           12
       13.732           48     6984.553     0.525808           21           15            8
       13.732           24        0.000     0.556326           21           17            0
       13.732           24        0.000     0.520802           27            1            0
       13.769           48      805.905     0.956158           18           17           11
       13.769           48     3654.744     0.365521           19           18            7
       13.769           48    11134.515     0.429707           21           17            2
       13.769           48      514.928     1.084913           22           13            9
       13.769           48     1388.901     0.841474           22           15            5
       13.769           48     5090.758     0.680468           23           13            6
       13.769           48      118.760     1.919536           23           14            3
       13.769           48     2065.000     0.778836           25           10            3
       13.769           48     1673.389     0.810194           26            7            3
       13.769           48     1752.430     0.304277           27            2            1
       13.788           48      115.481     0.140374           24           12            4
       13.807           48    13001.454     0.522117           19           16           11
       13.807           24        0.000     0.550671           19           19            4
       13.807           24        0.000     0.644168           20           13           13
       13.807           48     3757.070     0.522116           20           17            7
       13.807           24        0.000     0.619965           24            9            9
       13.807           48      166.534     0.522118           25            8            7
       13.807           24        0.000     0.642318           27            3            0
       13.825           48      432.177     0.521196           20           14           12
       13.825           48    12337.985     0.521198           20           18            4
       13.825           24     6312.746     0.521198           22           16            0
       13.825           48     1634.139     0.521198           24           10            8
       13.825           24     6345.703     0.521198           26            8            0
       13.844           48     1706.373     0.805092           25            9            6
       13.844           48     3221.206     0.721440           27            3            2
       13.863           48     3274.244     0.263069           22           14            8
       13.863           48     3664.048     0.274854           22           16            2
       13.863           48     4512.130     0.805788           26            8            2
       13.881           48      202.873     0.518453           20           15           11
       13.881           48       53.521     0.518447           21           16            7
       13.881           48      164.154     0.518448           21           17            4
       13.881           48     4790.123     0.518451           24           11            7
       13.881           48      143.928     0.518449           24           13            1
       13.881           24        0.000     0.551518           25           11            0
       13.881           48     5639.001     0.518451           27            4            1
       13.900           24        0.000     0.480472           18           18           10
       13.900           24        0.000     0.536103           26            6            6
       13.919           48     4715.988     0.374636           19           17           10
       13.919           48     1152.720     0.252972           23           11           10
       13.919           48    14412.105     0.608090           23           14            5
       13.919           48     8711.256     0.409941           25           10            5
       13.919           48    12031.894     0.425067           25           11            2
       13.919           48      997.063     0.904037           26            7            5
       13.956           48     1712.422     0.514812           21           13           12
       13.956           48       51.106     0.514808           23           12            9
       13.956           24        0.000     0.493669           23           15            0
       13.956           48     3151.326     0.514811           24           13            3
       13.956           48     4966.151     0.514812           27            4            3
       13.956           24        0.000     0.544797           27            5            0
       13.974           48   184851.469     0.560507           20           16           10
       13.974           48    70229.789     0.590530           22           16            4
       13.974           48   102809.844     0.576854           24           12            6
       13.974           48    77585.695     0.586684           26            8            4
       13.993           24    27149.818     0.579212           19           19            6
       13.993           48     2431.204     0.749978           21           14           11
       13.993           48    34488.859     0.457621           22           15            7
       13.993           48      364.326     0.108468           23           15            2
       13.993           48     1418.150     0.270548           26            9            1
       13.993           48     9578.805     0.410609           27            5            2
       14.011           48    46500.246     0.523157           20           18            6
       14.030           48        0.084     0.511293           20           19            1
       14.030           48     3199.971     0.511198           23           13            8
       14.030           48    13297.949     0.511198           25           11            4

-------------- next part --------------
/*******************************************************************************
*
* McStas, version 1.2 released February 2000
*         Maintained by Kristian Nielsen and Kim Lefmann,
*         Risoe National Laboratory, Roskilde, Denmark
*
* %IDENTIFICATION
*
* Author: <a href="mailto:hansen at ill.fr">Thomas C Hansen</a>
* Date: 08 March 2000
* Version: $Revision: 1.1 $
* Origin: <a href="http://www.ill.fr">ILL</a> (Dif/<a href="http://www.ill.fr/YellowBook/D20">D20</a>)
*
* General powder sample in incoherent scattering cylindrical can
*
* %DESCRIPTION
*
* This is a general powder sample in incoherent scattering cylindrical vanadium can.
* It creates elastic coherent scattering from a table of structure factors and incoherent
* background scattering from the sample itself and its container. To be efficient, the
* component is focussing on a given target, normally corresponding to a PSD or a multi-
* detector bank. Absorption is considered, as well attenuation of the beam, so the 
* probability of scattering is higher closer to the incoming beam. Multiple scattering
* (and so secondary extinction) is not considered yet, nor diffuse scattering, or elastic
* coherent scattering from a sample can, nor any inelastic scattering or elastic scattering 
* from amorphous materials. It is planned to implement multiple scattering and elastic
* coherent scattering from the sample can in the near future. Transmitted neutrons are
* normally not created, but only scattered neutrons leaving towards the detector target.
*
* %PARAMETERS
*
* INPUT PARAMETERS
*       
* radius:	(m)		Radius of sample in (x,z) plane 									(0.005)    
* h: 		(m)		Height of sample y direction 										(0.05)
* pack:		(1)		Packing factor 												(1)
* Vc:		(AA**3) 	Volume of unit cell
* sigma_a:	(fm**2)		Absorption cross section per unit cell at 2200 m/s
* j:		(*1)		Array of multiplicities
* q:		(*1/AA)		Array of wavevectors
* F2:		(*fm**2)	Array of structure factors
* DW:		(*1/AA**2)	Array of Debye-Waller factors
* write:	(1)		Output flag for writing in file sample.dat 								(0)
* transmission:	(1)		Ratio of transmitted neutron histories 									(0)
* nbInt:	(1)		Number of Bragg relections (size of the arrays)
* sigma_i:	(fm**2)		Incoherent scattering cross section of the sample per unit cell
* d_V:		(m) 		Thickness of the Vanadium sample can 									(0.0001) 
* broadening:	(1)		FWHM of the lattice constant variations for strain broadening 						(0)
* ttmin:	(deg)		Minimum 2theta angle of target <a href="../monitors/PSD_curved.html">PSD_curved.comp</a>		(0)
* ttmax:	(deg)		Maximum 2theta angle of target <a href="../monitors/PSD_curved.html">PSD_curved.comp</a>		(156.36)
* PSD_r:	(m)		Radius of curved linar PSD target <a href="../monitors/PSD_curved.html">PSD_curved.comp</a>		(1.471)
* PSD_h:	(m)		Height of curved linear PSD target <a href="../monitors/PSD_curved.html">PSD_curved.comp</a>		(0.15)
* sign:		(1)		Chirality of 1st diffractometer axis=sign[takeoff of <a href="../d20adapt.instr">d20adapt.instr]</a>	(-1)
*		
* OUTPUT PARAMETERS
*
* my_s_v2:	(m/s**2)	Attenuation factor due to elastic coherent scattering, multiplied by neutron velocity**2
* my_a_v:	(1/s)		Attenuation factor due to absorption, multiplied by neutron velocity
* q_v:		(m/s)		Corresponding velocity of wavevector Q
* my_i: 	(1/m)		Attenuation factor due to elastic incoherent scattering
*
* %LINKS
* <a href="../d20adapt.instr">Source code of d20adapt.instr</a>, where this component is used
* %LINKS
* A possible target detector: <a href="../monitors/PSD_curved.html">PSD_curved.comp</a>
* %LINKS
* <A HREF="http://neutron.risoe.dk/mcstas/components/Powder1/">The original component Powder1</A>, with explanation of focusing.
* %LINKS
* <A HREF="http://neutron.risoe.dk/mcstas/components/tests/powder/">Test results from Powder1</A> (not up-to-date).
*
* %END
*
*******************************************************************************/

DEFINE COMPONENT Powder0
DEFINITION PARAMETERS (radius, h, pack, Vc, sigma_a, j, q, F2, DW,write,transmission,nbInt,sigma_i,d_V,broadening,ttmin,ttmax)
SETTING PARAMETERS (PSD_r, PSD_h, sign)
OUTPUT PARAMETERS (my_s_v2, my_a_v, q_v,my_i)
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)
DECLARE
%{
#if __dest_os == __mac_os
	/* void Event_loop(); */
#endif
	double my_i;
 	unsigned long end_counter=0;  
  	double my_s_v2,my_s_v2_total, my_a_v, q_v;
  	double d_phi0,d_Scherrer,total_F2;
  	int    total,sign2,i;
  	FILE   *outfile;
	double V_pack=1.0;		/* Vanadium sample can */
	double V_sigma_a = 5.08;    	/* Absorption cross section per atom (barns) */
	double V_sigma_i = 4.935 ;  	/* Incoherent scattering cross section per atom (barns) */
	double V_rho   ; 		/* Density of atoms (AA-3) */
	double V_my_s ;
	double V_my_a_v,s ;
%}
INITIALIZE
%{
	V_rho    =(2.0 * V_pack/(3.024*3.024*3.024)); /* Density of atoms (AA-3) */
	V_my_s   =(V_rho * 100.0 * V_sigma_i);
	V_my_a_v =(V_rho * 100.0 * V_sigma_a * 2200.0);
	my_i=    sigma_i * pack/Vc *  100.0 ;
  	outfile=fopen("sample.dat","w");
  	my_a_v = sigma_a * pack/Vc * 2200.0;           /* Is not yet divided by v (which changes) */
  	my_s_v2_total=0.0;
  	for (i=1,my_s_v2=0.0, total_F2 = 0.0;(i<=nbInt);i++) 
  	{
	  if ((i<2)||(i>(nbInt-1))) printf("i=%4d Q=%9.2f j=%4d F2=%14.2f DW=%9.2f %9.5f\n",i,q[i],j[i],F2[i],DW[i],my_a_v);
  	}
  	d_phi0 = RAD2DEG*atan(0.5*(h+ PSD_h)/PSD_r);
  	total = 0;
  	printf("Vertical divergence (sample-PSD): %lfdeg, ",d_phi0);
  	printf("my(incoh.=)%lg/m, sigma(incoh.)=%lgbarn\n",my_i,sigma_i);
%}                                                                             
TRACE
%{
  double t20, t21,t2i0,t2i1,t0, t1,ti0,ti1, v, l_full,l_powder,l_can, l, l_1,l_2,l_p,l_c, dt, d_phi, theta, my_s, my,muR,muV;
  double aim_x, aim_y, aim_z, axis_x, axis_y, axis_z,my_total_powder,my_total_can;
  double tmp_vx, tmp_vy, tmp_vz, vout_x, vout_y, vout_z, Choice,total_F2_1,X;
  int i,coherent,powder;

  if (vz<0) ABSORB;
  my_s_v2_total=0.0;
  v = sqrt(vx*vx + vy*vy + vz*vz);	 	/* Very first, we should provide the neutron velocity ... */
  for (i=1,my_s_v2=0.0, total_F2 = 0.0;i<=nbInt;i++)  if (q[i]*K2V<(2.0*v))  
  {
  	my_s_v2_total += PI*PI*PI*pack*j[i]*F2[i]*DW[i]/(Vc*Vc*V2K*V2K*q[i]);	/* all 0 < 2theta < 180 deg */
      	if ((fabs(q[i]*K2V) < (sin(fabs(ttmax)/2*PI/180)*2.0*v))  &&  (fabs(q[i]*K2V) > (sin(fabs(ttmin)/2*PI/180)*2.0*v))) 
      	total_F2 += j[i]*F2[i]*DW[i]/q[i];	/* only ttmin < 2theta < ttmax */
  }
  total_F2_1=total_F2;
  total++;
  if (cylinder_intersect(&t0, &t1, x, y, z, vx, vy, vz, radius+d_V, h))
  {
   	if (t0 < 0) ABSORB; 			/* Neutron enters at t=t0. */
   	l_full = v * (t1 - t0);            	/* Length of full path through sample AND can - if there won't be any scattering */
   	if (rand01() < (double)transmission)  /* Transmission (IF any ...) */
   	{ 
 		my=my_i+my_a_v/v+my_s_v2_total/v/v; /* not exactly correct yet: considering can as sample ... */ 	
   		dt = l_full/v + t0;
     		PROP_DT(dt);
     		p*=exp(-my*l_full)/(double)transmission;
   	}
   	else 
   	{
   		/* Diffraction (elastic coherent AND incoherent scattering) */
   		/* it is sufficient to look here for choosing kind of scattering ... */
   		/* First, we must choose between scattering from sample or from container */
  		/* Therefore, we need (mu_i+mu_c)*R and mu_i(V)*d(V) and a random choice as done for coherent/incoherent */
  		/* To do it properly, we need the path of an unscattered neutron in Vanadium and in sample */
  		/* To do it even better, we may even consider 'multiple scattering', but that's valid for the sample itself beforehand ... */
  		if (cylinder_intersect(&ti0, &ti1, x, y, z, vx, vy, vz, radius, h))
  		{	
  			if (ti0 < 0) ABSORB; 
  			if (ti0 < t0) printf("\n%lg / %lg - %lg / %lg\n",t0,ti0,ti1,t1); 
  			l_powder = v * (ti1 - ti0);                      /* Length of full path through sample AND can */
 		} 
 		else 
 		{
 			ti0=(t0+t1)/2.0;
 			ti1=ti0;
 			l_powder=0.0;
 		}
 		if (ti0 < t0) printf("\n---> %12.6lg / %12.6lg - %12.6lg - %12.6lg / %12.6lg ---> %8.6lg %8.6lg %8.6lg - %8.6lg\n",t0,ti0,dt,ti1,t1,x,y,z,l_powder); 
 		l_can=l_full-l_powder;
  		muR=(my_s_v2_total/v/v+my_i)*l_powder;
  		muV=(V_my_s)*l_can;
  		Choice = fabs((muR+muV)*randpm1());
  		if (muR>=Choice) /****************** Scattering in Powder Sample ******************/
  		{
  			powder=1;
  			p*= (muR+muV)/muR ;
	  		/*** Now, we must choose between coherent or incoherent scattering ***/
  			Choice = fabs((my_s_v2_total/v/v+my_i)*randpm1());
  			if ((my_s_v2_total/(v*v))>=Choice) /****************** Coherent Scattering in Powder Sample ******************/
  			{	coherent=1;
  				if (ti0 < t0) printf("\n>>>> %lg / %lg - %lg / %lg\n",t0,ti0,ti1,t1); 
  				/**** In case of coherent scattering, choose a Bragg reflection ****/
  				total_F2=total_F2_1;
  				Choice = fabs(total_F2 * randpm1());
  				for (i=1,total_F2 = 0.0; i<=nbInt; i++)
  				{
  					if ((fabs(q[i]*K2V) < (sin(fabs(ttmax)/2*PI/180)*2.0*v))  &&  (fabs(q[i]*K2V) > (sin(fabs(ttmin)/2*PI/180)*2.0*v))) 
  					{
    	  					total_F2 += j[i]*F2[i]*DW[i]/q[i];
    	  					if (total_F2 >= Choice) 
    	  					{
    	    						break;
    	  					}
  					} 
  				}
  				/*printf("i=%3d, F2=%10.1lf, Q=%4.1lf, p=%10.2lg, ",i,F2[i],q[i],p);*/
  				if (i==0) i=1;
  				if (i>nbInt) i=nbInt;
  				p*=total_F2_1/(j[i]*F2[i]*DW[i]/q[i])*(my_s_v2_total/(v*v)+my_i)/(my_s_v2_total/(v*v)); 
   				/*printf("p=%10.2lg, ",p);*/
 				q_v = q[i]*K2V;
  				/* NEW: quick and dirty strain peak broadening (TH 22/10/99, mod 25/10/99) */
  				do
    				{
      					s = rand01();
      					s = 2*s - 1;
    				} while(s == 0);
  				X =sqrt(1.0/fabs(s)-1.0)/3.1415*s/fabs(s); /* Lorentzian distributuion */
  				q_v=1.0/(1.0/q_v*(1.0+broadening*X));
  				if ((2.0*v)<q_v) 
   				{
   					ABSORB; 
   				}
  				my_s_v2= PI*PI*PI*pack*j[i]*F2[i]*DW[i]/(Vc*Vc*V2K*V2K*q[i]); 
  				my=my_s_v2/v/v+my_a_v/v; 	/* my_s_v2 only known for coherent case */
  			}
  			else /****************** Incoherent Scattering in Powder Sample ******************/
  			{  	coherent=0;
  				my=my_i+my_a_v/v; 	
  				if (ti0 < t0) printf("\n===> %lg / %lg - %lg / %lg\n",t0,ti0,ti1,t1); 
  				/* in case of incoherent scattering choose random a scattering angle */
  				/* if ever possible choose it from the target solid angle ... but this will be difficult */
    				theta = (ttmin/2*+rand01()*(ttmax-ttmin)/2)*DEG2RAD;	/* Bragg scattering law */
    				q_v = sin(theta)*2.0*v; 		        /* Bragg scattering law */
  				/*printf("Incoherent in powder p=%10.2lg, ",p);*/
  				p*=(my_s_v2_total/(v*v)+my_i)/(my_i)*sin(2.0*theta);
  				/*printf("p=%10.2lg, ",p);*/
  				p*=PI/2*(-cos(fabs(ttmax/2)/180*PI)+cos(fabs(ttmin/2)/180*PI));
     				if (q[0]<0)
   		 		{	
   		 			theta = -theta;
    					q_v = -q_v;
    				}
  			}
   	 		dt = 1.0/my/v * -log(rand01()*(1-exp(-my*l_powder))+exp(-my*l_powder)) + ti0;
   	 		/* dt is NOT a difference, but the absolute time of scattering */
     			PROP_DT(dt);                		        /* Point of scattering */
			SCATTER;
     			l   = v*(dt -t0 );                   		/* Penetration in sample AND can */
    			l_c = v*(ti0-t0 );                   		/* Penetration in can */  			
			l_p = v*(dt -ti0);                   		/* Penetration in sample */
		}
		else /****************** Incoherent Scattering in Vanadium Sample Can ******************/
		{
			powder=0;
			p*= (muR+muV)/muV ;
			coherent=0; /* assume no Bragg scattering by Vanadium can - may be changed later! */
  			my=my_i+my_a_v/v; 	
  			/* in case of incoherent scattering choose random a scattering angle */
    			theta = (ttmin/2+rand01()*(ttmax-ttmin)/2)*DEG2RAD;	/* Bragg scattering law */
    			q_v = sin(theta)*2.0*v; 		        	/* Bragg scattering law */
  			/* printf("Incoherent in sample can: 2theta=%lf p=%10.2lg, ",2*theta/DEG2RAD,p); */
  			p*=sin(2.0*theta);
   			/* printf("p=%10.2lg, ",p); */
 			p*=PI/2*(-cos(fabs(ttmax/2)/180*PI)+cos(fabs(ttmin/2)/180*PI));
   			/* printf("p=%10.2lg, ",p); */
    			/* p is correct only if there is no elastic scattering */
    			if (q[0]<0)
   		 	{	
   		 		theta = -theta;
    				q_v = -q_v;
    			}
			/* simple choice, but modify p depending on scattering in entering or outgoing wall */
   	 		dt = rand01()*((t1-t0)-(ti1-ti0))+t0;
   	 		if (dt>ti0) dt+=(ti1-ti0);
     			PROP_DT(dt);                		/* Point of scattering */
			SCATTER;
     			l   = v*(dt -t0 );                   	/* Penetration in sample AND can */
     			if (dt>ti1) 
     			{
     				l_c = v*(dt - t0 - (ti1-ti0) );	/* Penetration in can */
     				l_p = v*(ti1-ti0); 
     			}
     			else 
     			{
     				l_c = v*(ti0-t0 );             	/* Penetration in can */
     				l_p = v*(dt -ti0);             	/* Penetration in sample */
			}
		}
	}
     	if (write>=1) fprintf(outfile,"%lf %lf %lf\n ", x,y,z);
     	theta = asin(q_v/(2.0*v)); 		        	/* Bragg scattering law */
     	d_Scherrer=2.0*PSD_r*sin(2.0*theta);
     	if (d_Scherrer<PSD_h) d_phi0 = 180.0;           	/* in this case take full cone! */
     	else d_phi0 = 2.0*RAD2DEG*asin(PSD_h/d_Scherrer); 	/* otherwise take only less than half of the cone */
     	d_phi  = d_phi0*DEG2RAD/2.0*randpm1();            	/* for very small scattering angles d_phi0 is variable ! */
     	p *= d_phi0/360.0; 
     	if (coherent == 0) i=0; 				/* not important, but must be an existing index ... */
     	if (q[i]<0) sign2=sign; 				/* we only consider an one-sided detector (in the higher resolution part) */
     	else 		sign2=-sign;
     	aim_x = (double)sign2*PSD_r*sin(2*theta)-x;       	/* Vector pointing at target (anal./det.) */
     	aim_y = -y ;
     	/* aim_z = fabs(PSD_r*cos(2*theta)-z); <- may be obsolete now */
     	aim_z = PSD_r*cos(2*theta)-z; /* the new way ... */
     	vec_prod(axis_x, axis_y, axis_z, vx, vy, vz, aim_x, aim_y, aim_z);
     	rotate(tmp_vx, tmp_vy, tmp_vz, vx, vy, vz, 2*theta, axis_x, axis_y, axis_z);
     	rotate(vout_x, vout_y, vout_z, tmp_vx, tmp_vy, tmp_vz, d_phi, vx, vy, vz);
     	vx = vout_x;
     	vy = vout_y;
     	vz = vout_z;
     	if(!cylinder_intersect(&t2i0, &t2i1, x, y, z,vout_x, vout_y, vout_z, radius, h)) /* a modifier ... */
     	{    
        	/* Do not exit here, the neutron may have hit only the wall of the sample can (TH 09/10/99) */ 
        	l_1=0.0; /* Only the sample can is hit by the neutron, there is not trace through the powder sample AFTER scattering */
    		l_2=0.0;
    		t2i0=0.0;
    		t2i1=0.0;
     	} 
     	else 
		{
	   		l_1 = v*t2i1; 		/* l_1 is the length of trace in the powder sample itself AFTER scattering */
	     	if (t2i0>0) 
	     	{
	     		l_2 = v*t2i0; 	/* l_3 is the length or trace in the entering wall of the sample can, after scattering */
	     		l_1-= v*t2i0;  	/* l_1 should not contain the part of the trace in the sample can if scattering happens in the entering wall */
	     	}
    	 	else l_2=0.0; 		/* l_3 should be zero if the powder itself scatters, or the exiting wall of the sample can */
	 	}
     	if(!cylinder_intersect(&t20, &t21, x, y, z,vout_x, vout_y, vout_z, radius+d_V, h)) /* a modifier ... */
     	{	 	
 			if (ti0 < t0) printf("\n---> %12.6lg / %12.6lg - %12.6lg - %12.6lg / %12.6lg ---> %8.6lg %8.6lg %8.6lg - %8.6lg\n",t0,ti0,dt,ti1,t1,x,y,z,l_powder); 
     		printf("\nCoherent: %d, powder: %d\n",coherent,powder);
			printf("%lg %lg %lg (%lg %lg) %lg %lg\n",t0,ti0,dt,ti1,t1,t21,t2i1);
     		printf("%6.1lf deg scattering angle (%lg, %d)\n", asin(q_v/(2.0*v))*2.0*RAD2DEG,q[i]*K2V,i);
     		printf("FATAL ERROR: Did not hit outer cylinder from inside.\n");
       		exit(1); /* This can really not happen ... at least, theoretically ... (TH 10/10/99) */
     	}
     	l_2 += v*(t21-t2i1);
	if (powder==0) 
	{
	 	my_s = V_my_s;
	 	l_full=l_can;
	}
	else
	{
	 	l_full=l_powder; 		
	    if (coherent==1) my_s = my_s_v2/(v*v);	/* my_s_v2 only known for coherent case */
    	 else my_s=my_i; 				/* of course ... even if it does not sound logic at the first glimpse */
	}	 
	/* l_full is now the full path without scattering through the finally scattering material, powder or can (TH 10/10/99) */
	my_total_powder=my_i+my_a_v/v+my_s_v2_total/(v*v);
	my_total_can   =V_my_s+V_my_a_v/v;
    	p *= fabs(l_full*my_s*exp(-my_total_powder*(l_p+l_1)-my_total_can*(l_c+l_2)))/(1.-(double)transmission); 
  	/*printf("%10.2lg, %10.2lg, p=%10.2lg\n",my_total_powder,my_s_v2_total,p);*/
	end_counter++;
    	/* if (p>1) exit(1); causes trouble with new source and weight>1*/
/*
	if ((unsigned long)fmod(end_counter,50) == 0)
    	{	
     		if (powder==0) printf("-"); 		
     		if (coherent==1) printf("*");		
     		else if (powder==1) printf("+");	
		fflush(stdout); 
#if __dest_os == __mac_os
	 Event_loop(); 
#endif
	}
*/
  }
  else ABSORB; /* ... if the neutron does not hit the sample ... */
%}
FINALLY
%{
  fclose(outfile);
  /*
  printf("\n");
  for (i=1;i<=nbInt;i++)
  {
	  printf("i=%4d N=%8d <P>=%18.15f \n",i,Nsum[i],Psum[i]/Nsum[i]);
  }
  */
%}

MCDISPLAY
%{
  magnify("xyz");
  circle("xz", 0,  h/2.0, 0, radius);
  circle("xz", 0, -h/2.0, 0, radius);
  circle("xz", 0,  h/2.0, 0, radius+d_V);
  circle("xz", 0, -h/2.0, 0, radius+d_V);
  line(-radius, -h/2.0, 0, -radius, +h/2.0, 0);
  line(+radius, -h/2.0, 0, +radius, +h/2.0, 0);
  line(0, -h/2.0, -radius, 0, +h/2.0, -radius);
  line(0, -h/2.0, +radius, 0, +h/2.0, +radius);
  line(-radius-d_V, -h/2.0, 0, -radius-d_V, +h/2.0, 0);
  line(+radius+d_V, -h/2.0, 0, +radius+d_V, +h/2.0, 0);
  line(0, -h/2.0, -radius-d_V, 0, +h/2.0, -radius-d_V);
  line(0, -h/2.0, +radius+d_V, 0, +h/2.0, +radius+d_V);
%}
END

-------------- next part --------------
/*******************************************************************************
*
* McStas, version 1.2 released February 2000
*         Maintained by Kristian Nielsen and Kim Lefmann,
*         Risoe National Laboratory, Roskilde, Denmark
*
* %IDENTIFICATION
*
* Written by: <a href="mailto:hansen at ill.fr">Thomas C Hansen</a>
* Date: 07 March 2000
* Version: $Revision: 1.0 $
* Origin: <a href="http://www.ill.fr">ILL</a> (Dif/<a href="http://www.ill.fr/YellowBook/D20">D20</a>)
*
* Pyrolytic graphite filter
*
* %DESCRIPTION
*
* This pyrolytic graphite filter, defined by two identical rectangular opening apertures, 
* is based upon empiric data and determines by
* interpolation the transmission of an incomming neutron, depending on its 
* wavelength. This type of filter is e.g. used to supress higher harmonics, so
* the 1.2 AA contribution to the 2.4 AA obtained by a highly orientated 
* pyrolytic graphite (HOPG) monochromator at a takeoff angle of 42 deg., as
* it is the case for the powder diffractometer D20 at the ILL Grenoble
*
* %PARAMETERS
*
* INPUT PARAMETERS:
*
* xmin: 	(m)	Lower x bound 			(-0.16)
* xmax: 	(m)	Upper x bound 			( 0.16)
* ymin: 	(m)	Lower y bound  			(-0.16)
* ymax: 	(m)	Upper y bound  			( 0.16)
* len:  	(m)	Thickness of graphite plate 	( 0.05)
*
* %LINKS
* <a href="../d20adapt.instr">Source code of d20adapt.instr</a>, where this component is used
* 
* %END
*
*******************************************************************************/

DEFINE COMPONENT Filter_Graphite
DEFINITION PARAMETERS (xmin, xmax, ymin, ymax, len)
SETTING PARAMETERS ()
OUTPUT PARAMETERS ()
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)
DECLARE
%{
%}
INITIALIZE
%{
%}
TRACE
%{
  double L,L1,L0,T1,T0, Filt_T;
  double dt;
  PROP_Z0;
  L = (2*PI/V2K)/sqrt(vx*vx + vy*vy + vz*vz);
  if (x<xmin || x>xmax || y<ymin || y>ymax) ABSORB;
  dt = len/vz;
  PROP_DT(dt);
  if (x<xmin || x>xmax || y<ymin || y>ymax) ABSORB;
  if (L>2.60) {L1= L  ;L0=2.60;T1=0.06;T0=0.06;}; 
  if (L<2.60) {L1=2.60;L0=2.40;T1=0.06;T0=0.05;}; 
  if (L<2.40) {L1=2.40;L0=2.30;T1=0.05;T0=0.09;}; 
  if (L<2.30) {L1=2.30;L0=2.20;T1=0.09;T0=0.22;}; 
  if (L<2.20) {L1=2.20;L0=2.00;T1=0.22;T0=0.34;}; 
  if (L<2.00) {L1=2.00;L0=1.90;T1=0.34;T0=0.61;}; 
  if (L<1.90) {L1=1.90;L0=1.80;T1=0.61;T0=0.23;}; 
  if (L<1.80) {L1=1.80;L0=1.60;T1=0.23;T0=0.25;}; 
  if (L<1.60) {L1=1.60;L0=1.40;T1=0.25;T0=0.27;}; 
  if (L<1.40) {L1=1.40;L0=1.30;T1=0.27;T0=0.53;}; 
  if (L<1.30) {L1=1.30;L0=1.20;T1=0.53;T0=0.98;}; 
  if (L<1.20) {L1=1.20;L0=1.10;T1=0.98;T0=0.89;}; 
  if (L<1.10) {L1=1.10;L0=1.00;T1=0.89;T0=0.52;}; 
  if (L<1.00) {L1=1.00;L0=0.87;T1=0.52;T0=0.47;}; 
  if (L<0.87) {L1=0.87;L0= L  ;T1=0.47;T0=0.47;}; 
  Filt_T=(T0+(L-L0)/(L1-L0)*(T1-T0))*100.0;
  Filt_T = exp(-Filt_T*len);
  p*=Filt_T;
%}
FINALLY
%{
%}
MCDISPLAY
%{
  magnify("xy");
  multiline(5, (double)xmin, (double)ymin, 0.0,
               (double)xmax, (double)ymin, 0.0,
               (double)xmax, (double)ymax, 0.0,
               (double)xmin, (double)ymax, 0.0,
               (double)xmin, (double)ymin, 0.0);
  multiline(5, (double)xmin, (double)ymin, (double)len,
               (double)xmax, (double)ymin, (double)len,
               (double)xmax, (double)ymax, (double)len,
               (double)xmin, (double)ymax, (double)len,
               (double)xmin, (double)ymin, (double)len);
  line(xmin, ymin, 0.0, xmin, ymin, len);
  line(xmax, ymin, 0.0, xmax, ymin, len);
  line(xmin, ymax, 0.0, xmin, ymax, len);
  line(xmax, ymax, 0.0, xmax, ymax, len);
%}
END

-------------- next part --------------
/*******************************************************************************
*
* McStas, version 1.2 released February 2000
*         Maintained by Kristian Nielsen and Kim Lefmann,
*         Risoe National Laboratory, Roskilde, Denmark
*
* %IDENTIFICATION
*
* Written by: <a href="mailto:hansen at ill.fr">Thomas C Hansen</a>
* Date: 08 March 2000
* Version: $Revision: 2.0 $
* Origin: <a href="http://www.ill.fr">ILL</a> (Dif/<a href="http://www.ill.fr/YellowBook/D20">D20</a>)
*
* Non-flat monochromator crystal with multiple scattering
*
* %DESCRIPTION
*
* Non-flat monochromator which uses a small-mosity approximation as well as
* the approximation vy^2 << vz^2 + vx^2. The crystal may be in transmission 
* geometry as well as in reflection. Multiple scattering is possible. The
* individual reflectivity for each neutron is calculated from its velocity
* vector, the structure factor of the monochromator crystal and its mosaic.
* For an unrotated monochromator component, the crystal plane lies in the y-z
* plane (ie. parallel to the beam).
*
* %PARAMETERS
* 
* INPUT PARAMETERS:
*
* xmin:		(m)		Lower x-bound of crystal 
* xmax:		(m)		Upper x-bound of crystal 
* zmin:		(m)		Lower z-bound of crystal 
* zmax:		(m)		Upper z-bound of crystal 
* ymin:		(m)		Lower y-bound of crystal 
* ymax:		(m)		Upper y-bound of crystal 
* mosh:		(min)		Horizontal mosaic (FWHM)
* mosv:		(min)		Vertical mosaic (FWHM) 
* dist:		(m)		Distance from target (sample), not yet used (17.2)
* xw:		(m)		Width of target (sample), not yet used (0.01)
* write:	(1)		Flag (1/0) to write debugging information in a file
* F2:		(fm**2)		Structure factor of monochromator material
* Vc:		(AA**3)		Unit cell volume of monochromator material
* omega:	(deg)		Rocking angle difference from Bragg reflection position (0)
* Q:		(1/AA)		Wavevector of scattering
* harmonic:	(1)		Order of first higher, contamining harmonic (2 for Cu or HOPG, 3 for Ge)
* B:		(1)		Debye-Waller factor of monochromator material
* LIMIT:	(1)		Upper limit of multiple scattering events to avoid infinite loops (1001)
* blade:	(1)		Number of blade in a focussing monochromator of several blades (0)
* present:	(1)		Flag (1/0) of presence of the component in focussing monochromators with variable number of elements (1)
*
* OUTPUT PARAMETERS:
*
* %LINKS
* <a href="../d20adapt.instr">Source code of d20adapt.instr</a>, where this component is used
* 
* %END
*
*******************************************************************************/

DEFINE COMPONENT Monochromator0
DEFINITION PARAMETERS (xmin, xmax, zmin, zmax, ymin, ymax, mosh, mosv, dist, xw, write, F2, Vc, omega, Q, harmonic, B, LIMIT,blade, present)
SETTING PARAMETERS ()
OUTPUT PARAMETERS ()
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)
DECLARE
%{
    #define DIV_CUTOFF 2            /* ~ 10^-5 cutoff. */
    	double d0,my,tmp7,tmp8;
    	int    z_edge,x_edge;
    	int    z_edge0,x_edge0;
    	int    counter;
%}
INITIALIZE
%{	
	/*
	double my,r0,l,Mono_d,v;
	*/
  	tmp7=0;
	tmp8=0;
    	z_edge=0;
    	x_edge=0;
    	counter=0;
	fprintf(monofile,"p0,r0, my0, l0, phi0,p1,r1,p2,vx2,vy2\n");
  	/*
      	v = sqrt(vx*vx+vy*vy+vz*vz);
	Mono_d = 2*PI/Q;
      	my = PI*PI*PI*2.0*F2*exp(-Mono_B/4.0/Mono_d/Mono_d)/(Vc*Vc*V2K*V2K*Q)/v/v*(360*360*60*60/mosh/mosv/PI);
	l=xmax-xmin;
	if (l > (zmax-zmin)) l=zmax-zmin;
   	r0=1.0-exp(-my*l);
	printf ("Monochromator: my=%lf/cm => R=%lf percent for l=%lfmm and v=%lfm/s\n",my/100,r0*100,l*1000,v);
	*/
%}                                                                             
TRACE
%{
    double dphi,tmp1,tmp2,tmp3,tmp4,tmp5,tmp6,vratio,phi,theta0,theta,v,cs,sn;
    double old_x = x, old_y = y, old_z = z, old_t = t, old_vx=vx,old_vz=vz, tmp_vx=vx,tmp_vz=vz;
    double dt, dtx,dty,dtz,l, r0,q,l_total,tmp_x,tmp_y,tmp_z;
    double new_x,new_y,new_z,new_t;
    int j;

  old_x=x; old_y=y;old_z=z;old_t=t;
  if (present)
  {
    if (vx == 0.0) dtx=0.; else if ((xmin-x)/vx > (xmax-x)/vx) dtx = (xmax-x)/vx; else dtx = (xmin-x)/vx;
    if (vy == 0.0) dty=0.; else if ((ymin-y)/vy > (ymax-y)/vy) dty = (ymax-y)/vy; else dty = (ymin-y)/vy;
    if (vz == 0.0) dtz=0.; else if ((zmin-z)/vz > (zmax-z)/vz) dtz = (zmax-z)/vz; else dtz = (zmin-z)/vz;
    if (dtx > dtz) dt=dtx; else dt=dtz;
    if (dty > dt ) dt=dty;
    new_x = x+vx*dt; new_y = y+vy*dt; new_z = z+vz*dt; new_t = t+dt;
    if (new_x>=xmin-0.000001 && new_x<=xmax+0.000001 && new_z>=zmin-0.000001 && new_z<=zmax+0.000001 && new_y>=ymin-0.000001 && new_y<=ymax+0.000001)
    {   
        x=new_x;y=new_y;z=new_z;t=new_t;
      	counter++;
      	if ((int)write == 1) 
      	{
              if (fabs(x-xmin)<.000001) 
                x_edge++; 
              if (fabs(z-zmin)<.000001) 
                z_edge++; 
      	}
      	if (vx == 0.0) dtx=0; else if ((xmin-x)/vx < (xmax-x)/vx) dtx = (xmax-x)/vx; else dtx = (xmin-x)/vx;
      	if (vy == 0.0) dty=0; else if ((ymin-y)/vy < (ymax-y)/vy) dty = (ymax-y)/vy; else dty = (ymin-y)/vy;
      	if (vz == 0.0) dtz=0; else if ((zmin-z)/vz < (zmax-z)/vz) dtz = (zmax-z)/vz; else dtz = (zmin-z)/vz;
      	if (dtx < dtz) dt=dtx; else dt=dtz;
      	if (dty < dt ) dt=dty;
	if (dt>0)
	 {
      		v = sqrt(vx*vx+vy*vy+vz*vz);
      		/* First: scattering in plane */
      		theta0 = atan2(vx,vz)-omega*PI/180;           	/* neutron angle to slab */
      		/* if(theta0 < 0) theta = -theta; - useless statement ... but, careful, why has it been written once? ... */
      		theta  = asin(Q2V*Q/(2.0*v));                  	/* Bragg's law */
   		if (counter <0) printf("Theta0=%lf, Theta=%lf (%lf), Omega=%lf, ",theta0*180/PI,theta*180/PI,Q2V*Q/(2.0*v), omega); 
      		tmp3 = (theta-theta0)/(MIN2RAD*mosh);
      		theta  = (Q2V*Q*(double)harmonic/(2.0*v));    	/* Bragg's law */
      		if (theta>1) theta=asin(1); 
      		else theta  = asin(theta);                  	/* Bragg's law */
   		if (counter <0) printf("for %d.harmonic: Theta=%lf (%lf)",harmonic,theta*180/PI,Q2V*Q*(double)harmonic/(2.0*v)); 
      		if (fabs(tmp3)>fabs((theta-theta0)/(MIN2RAD*mosh))) q=Q*(double)harmonic;
      		else q=Q;
      		theta  = asin(Q2V*q/(2.0*v));                  	/* Bragg's law */
      		tmp3 = (theta-theta0)/(MIN2RAD*mosh);
  		Mono_d = 2*PI/q;
   		if (counter <0) if (q!=Q) printf(" *"); 
   		if (counter <0) printf("\n");  
      		l = v * dt;
      		l_total=l;
  		tmp4=exp(-tmp3*tmp3*4*log(2)); /*** the relative orientation goes into the calculation of my !!!(?) ******/
        	phi  = atan2(vy,vz);           /* ... but not the out-of plane angle! (? - because this will change with multiple scattering) */
      		my = tmp4*PI*PI*PI*2.0*F2*exp(-B/4.0/Mono_d/Mono_d)/(Vc*Vc*V2K*V2K*q)/v/v*(360*360*60*60/mosh/mosv/PI);
      		/* 
			my = tmp4*PI*PI*PI*2.0*F2*exp(-Mono_B/4.0/Mono_d/Mono_d)/(Vc*Vc*V2K*V2K*q)/v/v*(360*60/mosh/PI);
		*/
		/* Reflectivity r0 */
   		r0=1.0-exp(-my*l/**exp(-phi*phi*4*log(2)/(MIN2RAD*mosv)/(MIN2RAD*mosv))*/);
   		if ((counter <0)||(r0<0)) printf("F2=%lf, Vc=%lf, mosh=%lf, mosv=%lf\n",F2,Vc,mosh,mosv); 
   		if ((counter <0)||(r0<0)) printf("v=%lfm/s, Q=%lf/AA\nMu=%lf/mm, path=%10.2lgmm, ",v,q,my/1000,l*1000); 
   	  	if ((counter <0)||(r0<0)) printf("MuR=%lf, Reflectivity=%10.2lg, Transmission=%lg, time= %lf s\n",my*l,100*r0,100*(1-r0),dt); 
   	  	d0 =1-r0;
   	  	d0+=rand01()*r0;
   	  	if ((counter <0)||(r0<0)) printf("Transmission at point of scattering: %lg, ",d0*100); 
   	  	d0 =-log(d0);
   	  	d0/=my;
   	  	dt=d0/v;
   	  	if (counter <0) printf("\nEnter at x=%lgmm, z=%lgmm",x*1000,z*1000); 
   	  	tmp_x=x; tmp_y=y; tmp_z=z;
      		x += vx*dt; y += vy*dt; z += vz*dt; t += dt;
   	  	l_total = sqrt((x-tmp_x)*(x-tmp_x)+(y-tmp_y)*(y-tmp_y)+(z-tmp_z)*(z-tmp_z));
		fflush(monofile);
   	  	if (counter <0) printf("\nScattering at %lgmm, time=%lgs, x=%lgmm, z=%lgmm\n",d0*1000,dt,x*1000,z*1000); 
       		if ((int)write == 1) if (counter < 1e4) fprintf(monofile,"%lf\n", p); 
      		/* First: scattering in plane */
      		if(fabs(tmp3) > DIV_CUTOFF)
      		{
        		x = old_x; y = old_y; z = old_z; t = old_t;
      		}
      		else
      		{
    	  	SCATTER;
			if (counter < 1e4) fprintf(monofile,"%12lg %12lg %12lg %12lg %12lg ",p,r0, my, l, phi);
 			if (r0<0) printf("p_in=%10.2lg, ",p);
			incident_p+=p;
        		p *= r0;
			first_p+=p;
			if (counter < 1e4) fprintf(monofile,"%12lg ",p);
        		/* p *= tmp4;  we consider this already in the calculation of my, don't we? */
        		tmp1 = 2*theta;
        		tmp6=1;
        		cs = cos(tmp1);
        		sn = sin(tmp1);
        		tmp2 = cs*vx - sn*vz; 
   	  	 	if (counter <0) printf("vx=%lgm/s, vz=%lgm/s =>",vx,vz); 
        		old_vz=vz; 					/***** NEW! *****/
        		old_vx=vx; 					/***** NEW! *****/
       	 		vy = vy;
        		vz = cs*vz + sn*vx; 
        		vx = tmp2;
   	  	   	if (counter <0) printf("vx=%lgm/s, vz=%lgmm\n",vx,vz); 
        		/* Second: scattering out of plane. **********************************/
           		/* Approximation is that Debye-Scherrer cone is a plane **************/
        		phi = atan2(vy,vz);                            /* out-of plane angle */
        		dphi = (MIN2RAD*mosv)/(2*sqrt(2*log(2)))*randnorm();  /* MC choice: **/
        		/* Vertical angle of the crystallite */
        		vy = vz*tan(phi+2*dphi*sin(theta));
        		vratio = v/sqrt(vx*vx+vy*vy+vz*vz);
        		vz = vz*vratio;
        		vy = vy*vratio;                             /* Renormalize v */
        		vx = vx*vratio;
      			/***************** NEW: MULTIPLE SCATTERING ************************************************************************/
      			j=1;
      			if (vx == 0.0) dtx=0; else if ((xmin-x)/vx < (xmax-x)/vx) dtx = (xmax-x)/vx; else dtx = (xmin-x)/vx;
      			if (vy == 0.0) dty=0; else if ((ymin-y)/vy < (ymax-y)/vy) dty = (ymax-y)/vy; else dty = (ymin-y)/vy;
      			if (vz == 0.0) dtz=0; else if ((zmin-z)/vz < (zmax-z)/vz) dtz = (zmax-z)/vz; else dtz = (zmin-z)/vz;
      			if (dtx < dtz) dt=dtx; else dt=dtz;
      			if (dty < dt ) dt=dty;
      			l = v * dt;
      			tmp5=rand01();
   	  		r0=1.0-exp(-my*l/**exp(-phi*phi*4*log(2)/(MIN2RAD*mosv)/(MIN2RAD*mosv))*/);
      			while (((tmp5<r0)||((j-2*(j/2))==0))&&(j<LIMIT))
      			{
      				j+=1;
   	  			d0 =1-r0;
     				if ((j-2*(j/2))==0) /* if neutron is about to leave in wrong direction, scatter it in any case and adjust probability ... */
      				{
      					p*=r0;
   	  				d0+=tmp5*r0;
      				}
      				else /* ... otherwise make a MC choice, also if limit has been passed */
      				{
   	  				d0=tmp5;
      				}
   	  			d0 =-log(d0);
   	  			d0/=my;
				if (d0 > l) break;
   	  			dt=d0/v;
   	  	 		if (counter <0) printf("Scattering at %lgmm, time=%lgs",d0*1000,dt); 
   	  	 		tmp_x=x; tmp_y=y; tmp_z=z;
      				x += vx*dt; y += vy*dt; z += vz*dt; t += dt;
      				SCATTER;
		   	  	l_total+= sqrt((x-tmp_x)*(x-tmp_x)+(y-tmp_y)*(y-tmp_y)+(z-tmp_z)*(z-tmp_z));
   	  	 		if (counter <0) printf(", x=%lgmm, z=%lgmm\n",x*1000,z*1000); 
   	  	 		tmp_vx=vx;
   	  	 		tmp_vz=vz;
        			vx=old_vx;
        			vz=old_vz;
        			old_vx=tmp_vx;
        			old_vz=tmp_vz;
        			phi = atan2(vy,vz);                            		/* out-of plane angle */
        			dphi = (MIN2RAD*mosv)/(2*sqrt(2*log(2)))*randnorm();	/* MC choice: **/
        			/* Vertical angle of the crystallite */
        			vy = vz*tan(phi+2*dphi*sin(theta));
        			vratio = v/sqrt(vx*vx+vy*vy+vz*vz);
        			vz = vz*vratio;
        			vy = vy*vratio;                             		/* Renormalize v */
        			vx = vx*vratio;
   	  	 		if (counter <0) printf("vx=%lgm/s, vz=%lgmm\n",vx,vz); 
      				if (vx == 0.0) dtx=0;  else if ((xmin-x)/vx < (xmax-x)/vx) dtx = (xmax-x)/vx; else dtx = (xmin-x)/vx;
      				if (vy == 0.0) dty=0;  else if ((ymin-y)/vy < (ymax-y)/vy) dty = (ymax-y)/vy; else dty = (ymin-y)/vy;
      				if (vz == 0.0) dtz=0;  else if ((zmin-z)/vz < (zmax-z)/vz) dtz = (zmax-z)/vz; else dtz = (zmin-z)/vz;
      				if (dtx < dtz) dt=dtx; else dt=dtz;
      				if (dty < dt ) dt=dty;
      				l = v * dt;
   			  	r0=1.0-exp(-my*l/**exp(-phi*phi*4*log(2)/(MIN2RAD*mosv)/(MIN2RAD*mosv))*/);
     				tmp5=rand01();
      			}
      			if (((vx*theta)>0)||(vx>0))
      			{
				if (counter < 1e4) fprintf(monofile,"%12lg %12lg %12lg %12lg\n",r0,p,vx,vz);
      				leaving_p+=p;
				ABSORB;
      			}
      			/****************** END OF MULTIPLE SCATTERING ***********************/
  			if (p<0) printf("r0=%10.2lg, tmp3=%10.2lg, p_out=%10.2lg\n",r0,tmp3,p);
 			leaving_p+=p;
			if (counter < 1e4) fprintf(monofile,"%12lg %12lg %12lg %12lg\n",r0,p,vx,vz);
			fflush(monofile);
      		}
     	}
      	else
      	{
      		/* x = old_x; y = old_y; z = old_z; t = old_t; */
      	}
    }
    else 
    {
      	/* x = old_x; y = old_y; z = old_z; t = old_t; */
    }
    if (counter<0) counter=0;
  } /* if present */
%}
FINALLY
%{
   	if ((int)write == 1) printf("x edge : %d neutrons, z edge : %d neutrons\n",x_edge ,z_edge );
%}
MCDISPLAY
%{
  magnify("xyz");
  multiline(16,(double)xmin*present, (double)ymin*present, (double)zmin*present,
               (double)xmin*present, (double)ymax*present, (double)zmin*present,
               (double)xmin*present, (double)ymax*present, (double)zmax*present,
               (double)xmin*present, (double)ymin*present, (double)zmax*present,
               (double)xmin*present, (double)ymin*present, (double)zmin*present,
               (double)xmax*present, (double)ymin*present, (double)zmin*present,
               (double)xmax*present, (double)ymax*present, (double)zmin*present,
               (double)xmin*present, (double)ymax*present, (double)zmin*present,
               (double)xmax*present, (double)ymax*present, (double)zmin*present,
               (double)xmax*present, (double)ymax*present, (double)zmax*present,
               (double)xmin*present, (double)ymax*present, (double)zmax*present,
               (double)xmax*present, (double)ymax*present, (double)zmax*present,
               (double)xmax*present, (double)ymin*present, (double)zmax*present,
               (double)xmin*present, (double)ymin*present, (double)zmax*present,
               (double)xmax*present, (double)ymin*present, (double)zmax*present,
               (double)xmax*present, (double)ymin*present, (double)zmin*present);
%}
END

-------------- next part --------------
/***********************************************************************
*
* McStas, version 1.2 released February 2000
*         Maintained by Kristian Nielsen and Kim Lefmann,
*         Risoe National Laboratory, Roskilde, Denmark
*
* %IDENTIFICATION
*
* Author: <a href="mailto:hansen at ill.fr">Thomas C Hansen</a>
* Date: 07 March 2000
* Version: $Revision: 1.0 $
* Origin: <a href="http://www.ill.fr">ILL</a> (Dif/<a href="http://www.ill.fr/YellowBook/D20">D20</a>)
*
* Curved linear 1D MSGC PSD
*
* %DESCRIPTION
*
* A curved linear 1D PSD monitor using a cylindrical projection. This detector type is commonly
* used in constant wavelength neutron powder diffraction, based either on multiwire- (MWGC) or
* microstrip- (MSGC) gaschamber technology. This implementation is mainly pushed by the MSGC
* realisation (D20) of such a PSD, as done on D20 at ILL. So some kind of 'polygonality' effect 
* resulting from the polygonal arrangement of MSGC plates will be considered in the near future
* by an approximation of the electron avalanche trace in the electrical field.
* 
* %PARAMETERS
*
* INPUT PARAMETERS:
*
* radius:	(m)		Radius of detector at center of MSGC plate (=radius in <a href="PSD_entry.html">PSD_entry</a> + gap)	(1.471)
* height:	(m)		Height of detector (=height in <a href="PSD_entry.html">PSD_entry</a>)					(0.15)
* nd:		(1)		Number of cells (=nd in <a href="PSD_entry.html">PSD_entry</a>)						(1536)
* pitch:	(deg)		angular pitch (=pitch in <a href="PSD_entry.html">PSD_entry</a>)					(0.1)
* gap:		(m)		gaschamber detection gap										(0.053)
* filename:	(string)	Name of file in which to store the detector image							(NULL)
* sign:		(1)		Chirality of 1st diffractometer axis=sign[takeoff of <a href="../d20adapt.instr">d20adapt.instr]</a>	(-1)
* tt0:		(deg)		Angular position of 1st PSD cell (=tt0 in <a href="PSD_entry.html">PSD_entry</a>)			(0)
* pdet:		(bar)		Pressure of 3He detection gas										(1.2)
* pT_trace:	(m)		Average effective length of proton/tritium trace							(0.005)
* period:	(1)		Number of detection cells per MSGC plate (=period in <a href="PSD_entry.html">PSD_entry</a>)		(32)
* cellwidth:	(m)		Width of one detection cell on a MSGC plate								(0.002568)
*
* OUTPUT PARAMETERS:
*
* PSD_N:    	(*1)		Array of neutron counts
* PSD_p:    	(*1.0)		Array of neutron weight counts
* PSD_p2:   	(*1.0)		Array of second moments
* alpha:	(rad)		Angle covered by one MSGC plate
* R1:		(m)		PSD radius at MSGC edge
*
* %LINKS
* <a href="../d20adapt.instr">Source code of d20adapt.instr</a>, where this component is used
* %LINKS
* <a href="PSD_entry.html">Source code of PSD_entry.comp</a>, a corresponding entry window
*
* %END
*
***********************************************************************/


DEFINE COMPONENT PSD_curved
DEFINITION PARAMETERS (	radius, height, nd, pitch, gap, filename, sign, tt0, pdet, pT_trace, period, cellwidth)
SETTING PARAMETERS ()
OUTPUT PARAMETERS (PSD_N, PSD_p, PSD_p2, alpha, R1)
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)
DECLARE
%{
  	int 	PSD_N[3601];
  	double 	PSD_p[3601];
  	double 	PSD_p2[3601];
	double  alpha, R1;
%}
INITIALIZE
%{
  int i;
  alpha=period*pitch/360.0*PI;
  R1=radius/cos(alpha);	
  for (i=0; i<nd; i++)
    {
      PSD_N [i] = 0;
      PSD_p [i] = 0;
      PSD_p2[i] = 0;
    }
%}
TRACE
%{
  double l,phi,v, l_full, t0, dt, t1, t2,t3, twotheta,eff,p_detection;
  double psi,theta, ax,ay,az, tx,ty,tz, ox,oy,oz, bx,by,bz;
  double x0,z0,R2,x1,z1,twotheta1,twotheta0,xp0,zp0,xp1,zp1,xx,zz,tmp;
  int    i0,i1,i,plate0,plate1;

  if(cylinder_intersect(&t0, &t1, x, y, z, vx, vy, vz, radius-gap, height) /* && t1 > 0 */)
  {
    	/*if(t0 < 0) t0 = t1;*/
    	if(t0 < t1) t0 = t1;
    	/*PROP_DT(t0);*/
	x+=vx*t0;
	y+=vy*t0;
	z+=vz*t0;
	t+=t0;
	SCATTER; /* incomming neutron */
	/* if ((double)sign*twotheta/PI*180. < tt0-pitch)        ABSORB; */
	/* if ((double)sign*twotheta/PI*180. > tt0+(nd+1)*pitch) ABSORB; */
	/* Polygonality effect in MSGC PSD - the detection gap is not really constant ... */
	/* Where would the n hit, if the outer radius is where the plates are closest to the entry */
    	cylinder_intersect(&t2, &t3, x, y, z, vx, vy, vz, radius, height);
    	if(t2 < 0) t2 = t3;
	x0=x+t3*vx;
	z0=z+t3*vz;
    	twotheta0 = -atan2(x0,z0);
     	i0 = floor(0.5+((double)sign*twotheta0/PI*180.0-tt0)/pitch);
	plate0=i0/period;
	/*
	printf("\nplate: %d, cell %d, twotheta %lf\n",plate0,i0,twotheta0/PI*180.0);
	*/
	/* Where would the n hit, if the outer radius is where two plates join */
    	cylinder_intersect(&t2, &t3, x, y, z, vx, vy, vz, R1, height);
    	if(t2 < 0) t2 = t3;
	x1=x+t3*vx;
	z1=z+t3*vz;
    	twotheta1 = -atan2(x1,z1);
    	i1 = floor(0.5+((double)sign*twotheta1/PI*180.0-tt0)/pitch);
	plate1=i1/period;	
	/*
	printf("plate: %d, cell %d, twotheta %lf\n",plate1,i1,twotheta1/PI*180.0);
	*/
	/* We try now to get the radius R2 where the n hits the plate */
  	twotheta=(tt0-pitch/2.0+(plate0+0.5)*period*pitch)*PI/180.0;
	/*
	printf("twotheta of plate %d: %lf\n",plate0,twotheta*180.0/PI);
  	*/
  	zp0=cos(twotheta-alpha)*R1;
	xp0=sin(twotheta-alpha)*R1;
	zp1=cos(twotheta+alpha)*R1;
	xp1=sin(twotheta+alpha)*R1;
	xx = (z0-(z1 -z0 )/(x1 -x0 )*x0) - (zp0-(zp1-zp0)/(xp1-xp0)*xp0);
	xx/=     (zp1-zp0)/(xp1-xp0)     -      (z1 -z0 )/(x1 -x0 );
	zz = (z0-(z1 -z0 )/(x1 -x0 )*x0) +      (z1 -z0 )/(x1 -x0 )     * xx ;
	/*
	printf("mt=%lf;bt=%lf \n",(z1 -z0 )/(x1 -x0 ),(z0 -(z1 -z0 )/(x1 -x0 )*x0 ));
	printf("mp=%lf;bp=%lf \n",(zp1-zp0)/(xp1-xp0),(zp0-(zp1-zp0)/(xp1-xp0)*xp0));
	printf("xx[0]=%lf;zz[0]=%lf\n",xx,zz);
	*/
	R2=sqrt(xx*xx+zz*zz);
	/*
	printf("R0=%lf;R1=%lf;R2=%lf\n",radius,R1,R2);
	printf("neutron hits plate %d (radius %lf < %lf < %lf) %lf %lf\n",plate0,radius,R2,R1,sqrt(x0*x0+z0*z0),sqrt(x1*x1+z1*z1));
	printf("twotheta = %lf to %lf\n",twotheta0/PI*180.0,twotheta1/PI*180.0);
	printf("plate %d (%lf,%lf) to (%lf,%lf)\n",plate0,xp0,zp0,xp1,zp1);
	printf("n hits between (%lf,%lf) and (%lf,%lf)\n",x0,z0,x1,z1);
	printf("%lf of plate \n",b);
	*/
	if (plate1 != plate0)
	{
  		twotheta=(tt0-pitch/2.0+(plate1+1)*period*pitch)*PI/180.0;
  		zp0=cos(twotheta-alpha)*R1;
		xp0=sin(twotheta-alpha)*R1;
		zp1=cos(twotheta+alpha)*R1;
		xp1=sin(twotheta+alpha)*R1;
		xx = (z0-(z1 -z0 )/(x1 -x0 )*x0) - (zp0-(zp1-zp0)/(xp1-xp0)*xp0);
		xx/=     (zp1-zp0)/(xp1-xp0)     -      (z1 -z0 )/(x1 -x0 );
		zz = (z0-(z1 -z0 )/(x1 -x0 )*x0) +      (z1 -z0 )/(x1 -x0 )     * xx ;
		tmp=sqrt(xx*xx+zz*zz);
		if (tmp<R2) 
		{
			R2=tmp;
			/*
			printf("neutron hits plate %d (radius %lf < %lf < %lf)\n",plate1,radius,R2,R1);
			*/
		}
		/*
		else printf("neutron hits plate %d (radius %lf < %lf < %lf)\n",plate0,radius,R2,R1);
		*/
	}
		if (R2 > R1) 
	{
		/*
		printf("neutron hits plate %d or %d (radius %lf < %lf < %lf)\n",plate0,plate1,radius,R2,R1);
		printf("##############################################################\n");
		*/
		R2=R1;
	}
	/* Now we got the virtual outer radius R2 which is in between 'radius' and 'R1' */
     	cylinder_intersect(&t2, &t3, x, y, z, vx, vy, vz, R2, height);
    	if(t2 < 0) t2 = t3;
	/* The following thing is not working as exspected to trace the trajectory of a neutron through the detection gap
    	PROP_DT(t2); 
    	SCATTER;               		
    	PROP_DT(-t2); 
    	SCATTER;               		
	*/
	x+=vx*t2;
	y+=vy*t2;
	z+=vz*t2;
	SCATTER;
	x-=vx*t2;
	y-=vy*t2;
	z-=vz*t2;
	SCATTER;
   	v = sqrt(vx*vx + vy*vy + vz*vz);
    	l_full = v * (t3);             /* Length of full path through sample */
	/*
	printf("Trajectory in gap %lfmm (%lf microsecs), ",l_full*1000,t3*1000000);
    	*/
    	eff=1.0-exp(-0.07417*pdet*l_full*100.0*VL/v);
    	dt = (t3) * -log(rand01()*(eff)+1.0-eff);/* + t0*/
	/*
	printf("efficiency %lf percent, capture after %lfmm\n",eff*100,dt*v*1000);
    	*/
    	PROP_DT(dt); 
    	SCATTER;               		/* Point of capture */
    	l = v*dt;                   	/* Penetration in detector */
    	p_detection=p*eff;
    	p*=1-eff;         /* a not detected (=captured) neutron may continue the flightpath!) */
    	/* Now, 2Theta for the place, where the neutron should have been detected ... */
	twotheta = -atan2(x,z);
	/* target vector b from neutron to PSD (in plane: y=0) */
	bx= sin(twotheta)*radius-x;
	by= 0.0;
	bz= cos(twotheta)*radius-z;
	/* axis a perpendicular to neutron vector v */
	vec_prod(ax,ay,az, vx,vy,vz,        bx,by,bz); 
	/* MC choice of angle component psi in a circle */
	psi  =2*PI*rand01();
	/* rotation in circle of neutron vector v around axis a (in plane) -> temporary trace vector t */
	rotate  (tx,ty,tz, vx,vy,vz, psi,   ax,ay,az);
	/* MC choice of second angle component in a sphere */
	theta=acos(randpm1());
	/* rotation in sphere of temporary trace vector t (out of plane) -> output pT trace vector o */ 
	rotate  (ox,oy,oz, tx,ty,tz, theta, vx,vy,vz);
	/* vx=ox;vy=oy;vz=oz;  - NOT the neutron changes it's direction but the pT trace o */
	NORM(ox,oy,oz);
	/* neutron is virtually detected at about a quarter of the total p/T trace length from capture */
	ox*=pT_trace/4.0;
	oy*=pT_trace/4.0;
	oz*=pT_trace/4.0;
	x+=ox;y+=oy;z+=oz;
	/* SHOW the part of pT trace leading to the point of virtual neutron capture detcted by the cas chamber PSD */
	SCATTER; 
	/* NOW 2Theta and phi is calculated for the gravicenter of electron avalanche */
    	twotheta = -atan2(x,z);
    	phi = asin(y/radius);
    	/* i = floor(0.5+(nx-1)*( (double)sign*twotheta/(2*PI) - tt0/360.)); */
     	i = floor(0.5+((double)sign*twotheta/PI*180.0-tt0)/pitch);
    	if ((i<nd && i>=0))
    	{
    	  	PSD_N [i] ++;
      		PSD_p [i] += p_detection;
      		PSD_p2[i] += p_detection*p_detection;
   	}
    	else 
    	{
    		ABSORB;
     	}
 }
 else 
 {
	ABSORB;
 }
 /* Yes, indeed, ABSORB IS a good idea for non-detected neutrons, as they do not interest anymore, and to use Check_adapt afterwards! */
%}
FINALLY
%{
  int i;
  double total=0.0,histories=0.0;
  char	string[40];
  
  for (i=0;i<nd;i++) 
  {
  	total+=PSD_p[i];
  	histories+=PSD_N[i];
  }
  sprintf(string,"Curved lin. PSD %9.4lgn/s (%8.3lg events)",total,histories);
  DETECTOR_OUT_1D(
        string,
        "2theta [deg]",
        "Intensity",
        "twotheta", tt0, tt0+nd*pitch, nd,
        &PSD_N[0],&PSD_p[0],&PSD_p2[0],
        filename);
%}

MCDISPLAY
%{
  double R2,x0,x1,z1,z0,twotheta,beta;
  int plate,cell;
  
  magnify("xyz");
  R1=radius/cos(period*pitch/360.0*PI);	
  for (plate=0;plate<ceil((double)nd/(double)period);plate++)
  {
  	twotheta=(tt0-pitch/2.0+(plate+0.5)*period*pitch)*PI/180.0;
	beta=atan(period/2.0*cellwidth/radius);
	R2=radius/cos(beta);
  	z0=cos(twotheta-beta)*R2;
	x0=sin(twotheta-beta)*R2;
	z1=cos(twotheta+beta)*R2;
	x1=sin(twotheta+beta)*R2;
  	line(x0,-height/2.0, z0,x1,-height/2.0, z1);
  	line(x0,+height/2.0, z0,x1,+height/2.0, z1);
  	line(x0,-height/2.0, z0,x0,+height/2.0, z0);
  	line(x1,-height/2.0, z1,x1,+height/2.0, z1);
	for (cell=0;cell<period;cell++)
	{
		circle("xz",x0+((double)cell+0.5)*(x1-x0)/(double)period,0,z0+((double)cell+0.5)*(z1-z0)/(double)period,cellwidth/2.0);
	}
  }
  R2=radius-gap;
  twotheta=(tt0-pitch/2.0)*PI/180.0;
  z0=cos(twotheta)*R2;
  x0=sin(twotheta)*R2;
  line(x0, -height/2.0,z0,x0, height/2.0,z0);
  for (cell=1;cell<=ceil((double)nd/(double)period)*period;cell++)
  {
  	twotheta=(tt0-pitch/2.0+pitch*cell)*PI/180.0;
	z1=cos(twotheta)*R2;
	x1=sin(twotheta)*R2;
	line(x0, -height/2.0,z0,x1, -height/2.0,z1);
	line(x0,  height/2.0,z0,x1,  height/2.0,z1);
	/* printf("%4d %10.5lf %10.5lf %10.5lf %10.5lf\n",cell ,x0,  z0,x1,z1);*/
  	x0=x1; z0=z1;
  }
  line(x0, -height/2.0,z0,x0, height/2.0,z0);
%}
END

-------------- next part --------------
/***********************************************************************
*
* McStas, version 1.2 released February 2000
*         Maintained by Kristian Nielsen and Kim Lefmann,
*         Risoe National Laboratory, Roskilde, Denmark
*
* %IDENTIFICATION
*
* Author: <a href="mailto:hansen at ill.fr">Thomas C Hansen</a>
* Date: 07 March 2000
* Version: $Revision: 1.1 $
* Origin: <a href="http://www.ill.fr">ILL</a> (Dif/<a href="http://www.ill.fr/YellowBook/D20">D20</a>)
*
* Entry window of a curved linear gaschamber PSD
*
* %DESCRIPTION
*
* Aluminium entry window for a curved linear position sensitive detector (PSD),
* as used in constant wavelength neutron powder diffraction (ILL Grenoble: D20).
* Normally, this component is always used in front of a <a href="PSD_curved.html">PSD_curved</a> component.
*
*
* %PARAMETERS
*
* INPUT PARAMETERS:
*
* radius:	(m)		Outer radius of detector entry window (=radius-gap in <a href="PSD_curved.html">PSD_curved</a>)		(1.418)
* height:	(m)		Height of detector (=height in <a href="PSD_curved.html">PSD_curved</a>)				(0.15)
* nd:   	(1)		Number of cells	(=nd in <a href="PSD_curved.html">PSD_curved</a>)					(1536)
* pitch:	(deg)		angular pitch (=pitch in <a href="PSD_curved.html">PSD_curved</a>)					(0.1)
* gap:		(m)		Thickness of entry window 										(0.007)
* tt0:		(deg)		detection angle of first cell (=tt0 in <a href="PSD_curved.html">PSD_curved</a>)			(0)
* pack:		(1)		Packing density of window material
* Vc:		(AA**3)		Unit cell volume of window material
* sigma_a:	(barn)		Absorption cross section
* q:		(1/AA)		Wavevector
* j:		(1)		Multiplicity
* F2:		(fm**2)		Structure factor
* DW:		(1/AA**2)	Debye-Waller factor
* period:	(1)		Number of cells on one MSGC plate (=period in <a href="PSD_curved.html">PSD_curved</a>)			(32)
* sign:		(1)		Chirality of 1st diffractometer axis=sign[takeoff of <a href="../d20adapt.instr">d20adapt.instr]</a>	(-1)
*
* OUTPUT PARAMETERS:
*
* my_s_v2:	(m/s**2)	Attenuation factor due to elastic coherent scattering, multiplied by neutron velocity**2
* my_a_v:	(1/s)		Attenuation factor due to absorption, multiplied by neutron velocity
* q_v:		(m/s)		Corresponding velocity of wavevector Q
*
* %LINKS
* <a href="../d20adapt.instr">Source code of d20adapt.instr</a>, where this component is used
* %LINKS
* The corresponding detector <a href="PSD_curved.html">PSD_curved.comp</<a>
* 
* %END
*
***********************************************************************/


DEFINE COMPONENT PSD_entry
DEFINITION PARAMETERS(radius,height,nd,pitch,gap,tt0,pack,Vc,sigma_a,q,j,F2,DW,period,sign)
SETTING PARAMETERS ()
OUTPUT PARAMETERS (my_s_v2, my_a_v, q_v)
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)
DECLARE
%{
  double my_s_v2, my_a_v, q_v;
%}
INITIALIZE
%{
  my_a_v = sigma_a/Vc*2200;           /* Is not yet divided by v */
  my_s_v2 = PI*PI*PI*pack*j*F2*DW/(Vc*Vc*V2K*V2K*q);  
  q_v = q*K2V;
%}
TRACE
%{
  double t0, t1, t2, t3, twotheta, d_phi, phi,eff,p_transmission;
  double my, l_full, dt, aim_x, aim_y, aim_z, axis_x, axis_y, axis_z;
  double l, tmp_vx, tmp_vy, tmp_vz, vout_x, vout_y, vout_z,v;
  int i;
  if(cylinder_intersect(&t0, &t1, x, y, z, vx, vy, vz, radius-gap, height) && t1 > 0)
  {
    if(t0 < 0) t0 = t1;
    PROP_DT(t0);
    /*SCATTER;*/
    twotheta = -atan2(x,z);
    /*printf("%lf\n",twotheta);*/
    if (((double)sign*twotheta>=tt0-pitch/2.0) && ((double)sign*twotheta<=tt0+(double)nd*pitch+pitch/2.0))
    {
      /*SCATTER;*/
      cylinder_intersect(&t2, &t3, x, y, z, vx, vy, vz, radius, height);
      if(t2 < 0) t2 = t3;
      v = sqrt(vx*vx + vy*vy + vz*vz);
      l_full = v * (t2);             /* Length of full path through PSD entry window of Al */
      my=my_s_v2/v/v+my_a_v/v;
      p_transmission=exp(-my*l_full);
      if (rand01() > p_transmission)
      {
        eff=1.0-exp(-my_s_v2/v/v*l_full);
        dt =(t2)*-log(rand01()*(eff)+1.0-eff);
        PROP_DT(dt);                		      /* Point of diffraction */
        l = v*dt;                   		      /* Penetration in entry window */
        p*=(eff)/(1-p_transmission);         /* a not detected (=captured) neutron may continue the flightpath!) */
        d_phi = 360.0*DEG2RAD/2.0*randpm1();
        twotheta = 2.0*asin(q_v/(2.0*v));  		/* Bragg scattering law */
        aim_x = sin(twotheta)-x;       		/* Vector pointing at target (anal./det.) */
        aim_y = -y ;/* + PSD_h/2*randpm1() ; doppelt wg. d_phi?*/
        aim_z = cos(twotheta)-z;
        vec_prod(axis_x, axis_y, axis_z, vx, vy, vz, aim_x, aim_y, aim_z);
        rotate(tmp_vx, tmp_vy, tmp_vz, vx, vy, vz, twotheta, axis_x, axis_y, axis_z);
        rotate(vout_x, vout_y, vout_z, tmp_vx, tmp_vy, tmp_vz, d_phi, vx, vy, vz);
        vx = vout_x;
        vy = vout_y;
        vz = vout_z;
      } 
      else 
      {
      	PROP_DT(t2);
	/*SCATTER;*/
      }
    }
    else ABSORB;
  }
  else ABSORB; 
  /* Yes, ABSORB is a good idea for non-detectedable neutrons, as they do not interest anymore, and to use Check_adapt afterwards! */
%}
FINALLY
%{
%}

MCDISPLAY
%{
  double R2, twotheta,x0,z0,x1,z1;
  int cell;
  
  magnify("xyz");
  R2=radius-gap;
  twotheta=(tt0-pitch/2.0)*PI/180.0;
  z0=cos(twotheta)*R2;
  x0=sin(twotheta)*R2;
  line(x0, -height/2.0,z0,x0, height/2.0,z0);
  for (cell=1;cell<=ceil((double)nd/(double)period)*period;cell++)
  {
  	twotheta=(tt0-pitch/2.0+pitch*cell)*PI/180.0;
	z1=cos(twotheta)*R2;
	x1=sin(twotheta)*R2;
	line(x0, -height/2.0,z0,x1, -height/2.0,z1);
	line(x0,  height/2.0,z0,x1,  height/2.0,z1);
  	x0=x1; z0=z1;
  }
  line(x0, -height/2.0,z0,x0, height/2.0,z0);
/* Circles are too roughly drawn for curved detector presentations */
/*
  circle("xz", 0,  height/2.0, 0, radius);
  circle("xz", 0, -height/2.0, 0, radius);
  line(-radius, -height/2.0, 0, -radius, +height/2.0, 0);
  line(+radius, -height/2.0, 0, +radius, +height/2.0, 0);
  line(0, -height/2.0, -radius, 0, +height/2.0, -radius);
  line(0, -height/2.0, +radius, 0, +height/2.0, +radius);
  circle("xz", 0,  height/2.0, 0, (radius-gap));
  circle("xz", 0, -height/2.0, 0, (radius-gap));
  line(-(radius-gap), -height/2.0, 0, -(radius-gap), +height/2.0, 0);
  line(+(radius-gap), -height/2.0, 0, +(radius-gap), +height/2.0, 0);
  line(0, -height/2.0, -(radius-gap), 0, +height/2.0, -(radius-gap));
  line(0, -height/2.0, +(radius-gap), 0, +height/2.0, +(radius-gap));
*/
%}
END

-------------- next part --------------
/***********************************************************************
*
* McStas, version 1.2 released February 2000
*         Maintained by Kristian Nielsen and Kim Lefmann,
*         Risoe National Laboratory, Roskilde, Denmark
*
* %IDENTIFICATION
*
* Author: <a href="mailto:hansen at ill.fr">Thomas C Hansen</a>
* Date: 07 March 2000
* Version: $Revision: 1.0 $
* Origin: <a href="http://www.ill.fr">ILL</a> (Dif/<a href="http://www.ill.fr/YellowBook/D20">D20</a>)
*
* Conversion from flat energy distribution to Maxwellian neutron spectra
*
* %DESCRIPTION
*
* The routine modifies/converts the incident flat (in energy) neutron spectra, 
* as it comes out from a source like the standard adaptive source 
* <a href="http://neutron.risoe.dk/mcstas/mcdoc/components/sources/Source_adapt.html">Source_adapt</a>, 
* to obtain a Maxwellian neutron distribution, as it is approximatively the case for thermal neutrons
* in a reactor's moderator (e.g. the HFR of the ILL in Grenoble). So, this 
* component is only a virtual one, not corresponding to a real element in a
* neutron beam.
*
* %PARAMETERS
*
* INPUT PARAMETERS:
*
* T:  	(K)	The temperature of the source, 293 K for thermal neutrons (beam tube H11 at ILL)
* E0:	(meV)	Mean energy of neutrons (as for <a href="http://neutron.risoe.dk/mcstas/mcdoc/components/sources/Source_adapt.html">Source_adapt</a>)
* dE: 	(meV)	Energy spread as for <a href="http://neutron.risoe.dk/mcstas/mcdoc/components/sources/Source_adapt.html">Source_adapt</a> (energy range is from E0-dE to E0+dE)
*
* OUTPUT PARAMETERS:
*
* Lmin:	(AA)	Minimum wavelength in energy range
* Lmax:	(AA)	Maxium wavelength in energy range
* l0:	(AA)	Mean wavelength of neutron spectra, about 1.8 AA for thermal neutrons
* L2P:	(AA**4)	Normalisation constant for Maxwell distribution
*
* %LINKS
* <a href="../d20adapt.instr">Source code of d20adapt.instr</a>, where this component is used
* %LINKS
* A source producing a flat in energy distribution: <a href="http://neutron.risoe.dk/mcstas/mcdoc/components/sources/Source_adapt.html">Source_adapt.comp</a>
*
* %END
*
***********************************************************************/

DEFINE COMPONENT Convert_FlatE_2_Maxwell
DEFINITION PARAMETERS (T,E0,dE)
SETTING PARAMETERS ()
OUTPUT PARAMETERS (Lmin,Lmax,l0,L2P)
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)
DECLARE
%{
  double l0, L2P, Lmin,Lmax;
	
%}
INITIALIZE
%{
  double k;
  k  = 1.38066e-23;
  l0=1.0e10*sqrt(HBAR*HBAR*4.0*PI*PI/2.0/MNEUTRON/k/T);	   
  L2P=2*l0*l0*l0*l0; 
  Lmin = sqrt(81.81/(E0+dE)); /* AAngstroem */
  Lmax = sqrt(81.81/(E0-dE));
%}
TRACE
%{
  double l,E, Maxwell,dE_dl;
  l= (2*PI/V2K)/sqrt(vx*vx + vy*vy + vz*vz);
  E=(VS2E*4.0*(PI*PI)/(V2K*V2K))/l/l;
  dE_dl=E/l*2.0;
  p*=2.0*dE/(Lmax - Lmin)/dE_dl; 
  Maxwell=L2P/l/l/l/l/l*exp(-l0*l0/l/l); 
  p*= Maxwell;
%}

FINALLY
  %{
  %}

MCDISPLAY
%{
  magnify("xy");
  circle("xy",0,0,0,0.1);
%}

END

-------------- next part --------------
/*******************************************************************************
*
* McStas, version 1.1, released 
*         Maintained by Kristian Nielsen and Kim Lefmann,
*         Risoe National Laboratory, Roskilde, Denmark
*
* Component: Hdiv_monitor
*
* Written by: KL,  Nov. 11, 1998
* Written by: Thomas Hhansen,  December, 1999
*
* A divergence sensitive monitor. The counts are distributed in 
* n pixels. 
*
* INPUT PARAMETERS:
*
* xmin:     Lower x bound of detector opening (m)
* xmax:     Upper x bound of detector opening (m)
* ymin:     Lower y bound of detector opening (m)
* ymax:     Upper y bound of detector opening (m)
* nh:       Number of pixel rows (1)
* h_maxdiv  Maximal vertical divergence detected (degrees)
* filename: Name of file in which to store the detector image (text)
*
* OUTPUT PARAMETERS:
*
* Div_N:    Array of neutron counts
* Div_p:    Array of neutron weight counts
* Div_p2:   Array of second moments
*
*******************************************************************************/


DEFINE COMPONENT Hdiv_monitor
DEFINITION PARAMETERS (xmin, xmax, ymin, ymax, 
                       nh, h_maxdiv, filename)
SETTING PARAMETERS ()
OUTPUT PARAMETERS (Div_N, Div_p, Div_p2) 
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)
DECLARE
  %{
    int Div_N[nh];
    double Div_p[nh];
    double Div_p2[nh];
  %}
INITIALIZE
  %{
    int i;

    for (i=0; i<nh; i++)
     {
/*       printf("HDiv_monitor: %d\n",i); */
      Div_N[i] = 0;
      Div_p[i] = 0;
      Div_p2[i] = 0;
     }
/*     printf("%d %d %d\n",i,nh,h_maxdiv); */
  %}
TRACE
  %{
    int i;
    double h_div;

    PROP_Z0;
    if (x>xmin && x<xmax && y>ymin && y<ymax)
    {
      h_div = RAD2DEG*atan2(vx,vz);
      if (h_div < (double)h_maxdiv && h_div > -(double)h_maxdiv)
      {
        i = floor((h_div + (double)h_maxdiv)*nh/(2.0*(double)h_maxdiv));
        Div_N[i]++;
        Div_p[i] += p;
        Div_p2[i] += p*p;
      }
    }
  %}
FINALLY
  %{
    DETECTOR_OUT_1D(
        "horizontal divergence monitor",
        "horizontal divergence [deg]",
        "Intensity",
        "divergence", -h_maxdiv, h_maxdiv, nh,
        &Div_N[0],&Div_p[0],&Div_p2[0],
        filename);
  %}

MCDISPLAY
  %{
    magnify("xy");
    multiline(5, (double)xmin, (double)ymin, 0.0,
                 (double)xmax, (double)ymin, 0.0,
                 (double)xmax, (double)ymax, 0.0,
                 (double)xmin, (double)ymax, 0.0,
                 (double)xmin, (double)ymin, 0.0);
%}


END

-------------- next part --------------
/*******************************************************************************
*
* McStas, version 1.0, released October 26, 1998
*         Maintained by Kristian Nielsen and Kim Lefmann,
*         Risoe National Laboratory, Roskilde, Denmark
*
* Component: PSD_bidim
*
* Written by: KL,  Feb 3, 1998 (PSD_monitor.comp)
* Rewritten by: Thomas Hansen, ILL Grenoble, France, 1999
*	Output modified
*
* An (n times m) pixel PSD monitor. This component may also be used as a beam
* detector.
*
* INPUT PARAMETERS:
*
* xmin:     Lower x bound of detector opening (m)
* xmax:     Upper x bound of detector opening (m)
* ymin:     Lower y bound of detector opening (m)
* ymax:     Upper y bound of detector opening (m)
* nx:       Number of pixel columns (1)
* ny:       Number of pixel rows (1)
* filename: Name of file in which to store the detector image (text)
*
* OUTPUT PARAMETERS:
*
* PSD_N:    Array of neutron counts
* PSD_p:    Array of neutron weight counts
* PSD_p2:   Array of second moments
*
*******************************************************************************/


DEFINE COMPONENT PSD_bidim
DEFINITION PARAMETERS (xmin, xmax, ymin, ymax, nx, ny, filename)
SETTING PARAMETERS ()
OUTPUT PARAMETERS (PSD_N, PSD_p, PSD_p2) 
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)
DECLARE
  %{
    int PSD_N[nx][ny];
    double PSD_p[nx][ny];
    double PSD_p2[nx][ny];
  %}
INITIALIZE
  %{
    int i,j;

    for (i=0; i<nx; i++)
     for (j=0; j<ny; j++) 
     {
      PSD_N[i][j] = 0;
      PSD_p[i][j] = 0;
      PSD_p2[i][j] = 0;
     }
  %}
TRACE
  %{
    int i,j;

    PROP_Z0;
    if (x>xmin && x<xmax && y>ymin && y<ymax)
    {
      i = floor((x - xmin)*nx/(xmax - xmin));
      j = floor((y - ymin)*ny/(ymax - ymin));
      PSD_N[i][j]++;
      PSD_p[i][j] += p;
      PSD_p2[i][j] += p*p;
    }
  %}
FINALLY
  %{
	int 	i,j,n=0;
	double 	flux=0.0,xx,yy,A;
	char	string[40];
	
	for (i=0; i<nx; i++)
	{
		xx=xmin+(xmax-xmin)*(double)i/(double)nx;
		for (j=0; j<ny; j++) 
		{
			yy=ymin+(ymax-ymin)*(double)j/(double)ny;
			if ((yy*yy+xx*xx)<=(0.01*0.01/PI)) 
			{	n++;
				flux +=PSD_p[i][j];
			}
		}
	}
	A=(double)n*(xmax-xmin)/(double)nx*(ymax-ymin)/(double)ny*100.0*100.0; /* cm2 */
	flux/=A;
	/* flux/=(double)created_neutrons; */
	sprintf(string,"BiDimPSD %9.4lgn/s/cm2",flux);
	DETECTOR_OUT_2D(
		string,
		"X position [cm]",
		"Y position [cm]",
		xmin*100.0, xmax*100.0, ymin*100.0, ymax*100.0,
		nx, ny,
		&PSD_N[0][0],&PSD_p[0][0],&PSD_p2[0][0],
		filename);
   
  %}

MCDISPLAY
%{
  magnify("xy");
  multiline(5, (double)xmin, (double)ymin, 0.0,
               (double)xmax, (double)ymin, 0.0,
               (double)xmax, (double)ymax, 0.0,
               (double)xmin, (double)ymax, 0.0,
               (double)xmin, (double)ymin, 0.0);
%}


END