General description
This file describes shortly a simulation packet based mainly on the HIJING 1.35 routines. It is intended to provide MC data needed to test efficiency of the PHOBOS detector. As an extension to standard HIJING it includes also a simple plasma source. I am going to include, in the near future, other new physical effects which would be relevant to our understanding of physics at RHIC energies.
The simulation packet includes:
The program is intended to compile and run on
Linux system with Portland compiler - pgf77, which is installed at RCF. It may also
work with g77 or egcs compiler after some modifications. To compile just type
'make'.
Control file
File 'hijing.dat' provides the main parameters
of a collision.
These are:
The number of run is given as a command line parameter. You can specify up to 30 runs. Note that the random number generator is initialized using current date and run number.
For the purpose of simulation at the RCF farm the program accepts the environment variable INPUT0, which sets the alternative name of the input file.
Output file
The results are put in the file 'hijing_yyyymmdd_#'
, where yyyymmdd stands for date and # is the current number of run. The output
contains header information which describes main parameters of the run and event. The
lines in the output file, which describe produced particles begin with 'P' and contain
GEANT parameters: ID of a particle, total momentum, theta and phi angles. The name of the
output file can be changed by setting the environment variable OUTPUT0.
Plasma source
In high energy collisions it is expected that some fraction of particles is produced directly from a plasma fireball. We decide to simulate this effect by random replacement of charged pions generated by HIJING by pions produced from thermal source. The main parameters are: temperature of the source T, which is estimated to be around 170 MeV, and probability pp of replacement of a pion. If pp=0 then we recover the pure HIJING results, on the other limit (pp=1.) we get the pure plasma source.
The total momentum of pions produced from plasma are distributed according to Boltzmann i.e.
n(p)/n(p')= (p^2/p'^2)*exp[ ( -E(p) + E(p') )/T ],
where n(p) is the number of particles produced with total momentum p.
Production of pions is assumed to be isotropic.
Obviously this model of plasma has several
restrictions and it will be a subject of further improvements.
If you have any comments contact:
Dr. Pawel Sawicki
High Energy Physics Lab
Institute of Nuclear Physics
ul. Kawiory 26a
30-055 Krakow
Poland
email : pawel.sawicki@ifj.edu.pl
tel. +12-48-6333366 (secr.)
fax. +12-48-6333884