The SHARE v. 2.1 program code and input files are contained
in a tar.gz archive (filename sharev2.1.tar.gz).
To unpack it, create a SHARE directory, put the archive
in it, and execute the following commands:

gunzip  sharev2.1.tar
tar -xf  sharev2.1.tar

The following files will then be created, enough for a
complete "representative" run of SHARE.
It should be noted that this run explores all of the calculational
potential of SHARE, including computations incorporating particle
widths.   Some of these, highlighted in the comments in the sharerun.data 
file, are very long (chi^2 profiles with particle widths could take hours).

The format of each file included is described in detail in the
SHAREv2.x paper, available at 
http://arXiv.org/abs/nucl-th/0603026
The SHAREv1.x manual is available at http://arxiv.org/abs/nucl-th/0404083 List of the files: decays.data The complete Particle Data Group decay tree (section 3.3 in v1.x manual) dec_no.data An empty decays file, useful for testing the program calculations (abundancies reduce to modified Bessel functions) as well as studying the role of resonances in stable particle ratios fortrat A shell script compiling (in f77) the FORTRAN code which should be modified depending on location of FORTRAN (g77 or f77) and CERN library of programs particles.data Particle properties, with full widths (section 3.2 in v1.x manual)) partnowdt.data Particle properties, with no widths. Calculations with this input file require considerably less computational time, and it suffices when there are no resonances in the fit. ratioset.data The FORTRAN fit input file (section 3.5 in v1.x manual) sharerun.data A "representative" run input file (section 4 in v1.x manual) including an analysis of fluctuations and yields similar to what was presented in QM2005, http://arXiv.org/abs/nucl-th/0509067 sharerun.data_onefile The same file in the "one file" format, as explained in section 4.1 of v2.x manual samplefit200 A directory containing the output files generated by running the provided "sharerun.data", as a debugging/comparison standard sharev2.1.f SHARE v2.1 FORTRAN code. The header contains information about bug fixes thermo.data A representative thermal parameter input file (section 3.1 in v1.x manual) It is set to reasonable non-equilibrium fit values totbar200.data A representative data input file (section 3.4 in v1.x manual) Containing: - ratios drawn from current (July 2004) RHIC experiments, http://arxiv.org/abs/nucl-ex/0403014. - Published yields of the Phi, http://arXiv.org/abs/nucl-ex/0406003 and pions, http://arxiv.org/abs/nucl-ex/0310004 - preliminary K/pi dynamical fluctuations, http://arXiv.org/abs/nucl-ex/0503023 When fitting from this input file, exact strangeness conservation is assumed. star.feed An example of a decay feed-down coefficients file. See v2.x manual section 2 fotrat A shell-script that compiles sharev2.1 Note that SHARE requires CERN libraries, to be downloaded separately from here. The compiler statement (in file "fortrat") is f77 -L/usr/local/cern/pro/lib -o sharev2.1.exe sharev2.1.f -lmathlib -lkernlib -lpacklib -C which assumes that the CERN libraries are in directory /usr/local/cern/pro/lib If this is not true on your system, fortrat should be changed accordingly. Once the directory is unpacked, the program should be compiled with ./fortrat After this, typing ./sharev2.1.exe should produce a correct run with a detailed output which shows the program's capability. Several output files are produced, with the following names as default. The contents of each file are explained in detail in section 4 of the paper. fit*.out Fit output files graph* Fit output graphics (experiment, fitted values, calculated values) ext*.out Extensive quantities calculated within the various models prof* Chi^2 profiles and correlation functions for the various fits *nwd*, *nowd* No width, strange and light non-equilibrium *width, *wd* Width, strange and light non-equilibrium *neq* No width, full equilibrium *weq* Width, full equilibrium *nweqs* No width, strangeness non-equilibrium *wdeqs* Width, strangeness non-equilibrium