- th / 9 90 60 65 v 1 2 2 Ju n 19 99 1 Particle Ratios at CERN , BNL and GSI : Unified description of Freeze - Out Parameters
نویسندگان
چکیده
It is shown that the chemical freeze-out parameters obtained at CERN/SPS, BNL/AGS and GSI/SIS energies all correspond to a unique value of 1 GeV for the average energy per hadron. Information about the chemical freeze-out parameters, the temperature, T ch , and baryon chemical potential µ ch B can be obtained from ratios of integrated particle yields [1,2]. This is because various effects like transverse flow or particle production from a superposition of fireballs cancel out in such ratios provided the freeze-out parameters are unique. We will discuss in succession particle ratios at GSI/SIS, BNL/AGS and SPS/CERN. We will then discuss common properties, in particular, the observation that all of them correspond to an average energy of 1 GeV per hadron independent of the beam energy [3]. A systematic study of the particle ratios measured at GSI/SIS energies has been done recently [4,5]. In figure 1 we show the results obtained in [5] for Ni-Ni at 1.0 AGeV. The particle ratios are consistent with the interpretation that the hadronic composition of the final state is fixed at a unique temperature and baryon chemical potential. Since the temperature is low, the number of particles created is small and it is therefore necessary to take into account the exact conservation of strangeness because strange particles are always produced in pairs and it is more difficult to create two particles in a small cold system than it is to create one particle. There is no necessity to introduce any other parameters and a good fit can be achieved with full chemical equilibrium including strange particles, i.e. with γ s = 1. In view of the fact that kaons are produced below threshold at SIS this is remarkable.
منابع مشابه
ar X iv : n uc l - th / 9 90 30 63 v 2 2 0 Ju l 1 99 9 Chemical and Thermal Freeze - Out Parameters
The present knowledge about hadrons produced in relativistic heavy ion collisions is compatible with chemical freeze-out happening when the energy density divided by the particle density reaches the value of 1 GeV. This observation is used to determine the energy dependence of the chemical freeze-out parameters Tch and μ ch B for beam energies varying between 1 and 200 A·GeV. The consequences o...
متن کاملar X iv : n uc l - th / 9 90 30 63 v 1 2 8 M ar 1 99 9 Chemical and Thermal Freeze - Out Parameters
The present knowledge about hadrons produced in relativistic heavy ion collisions is compatible with chemical freeze-out happening when the energy density divided by the particle density reaches the value of 1 GeV. This observation is used to determine the energy dependence of the chemical freeze-out parameters Tch and μ ch B for beam energies varying between 1 and 200 A·GeV. The consequences o...
متن کاملn uc l - th / 9 71 10 66 v 1 2 8 N ov 1 99 7 nucl - th / 9711066 Thermal Model Analysis of Particle Ratios at GSI Ni – Ni Experiments Using
The production of hadrons in Ni–Ni at the GSI is considered in a hadronic gas model with chemical equilibrium. Special attention is given to the abundance of strange particles which are treated using the exact conservation of strangeness. It is found that all the data can be described using a temperature T = 70± 10 MeV and a baryon chemical potential μB = 720± 20 MeV. Typeset using REVTEX 1
متن کاملMassive Constituent Quarks and Unified Description of Freeze-out Parameters: Does Qgp Form at Low Energies?
The possibility of unified description of hadron multiple production in heavy ion collisions over the wide energy interval, from few hundreds MeV/n at GSI/SIS through 11 GeV/n at BNL/AGS up to 160 GeV/n at CERN/SPS, has been emphasized recently by J. Cleymans and K. Redlich (CR) [1]. They, and somewhat later B. Muller and J. Rafelski [2], treated this fact as an indication that quark-gluon plas...
متن کاملar X iv : n uc l - th / 9 90 60 77 v 1 2 5 Ju n 19 99 NUCLEON - NUCLEON SCATTERING IN EFFECTIVE FIELD
I outline the effective field theory (EFT) calculation of nucleon-nucleon scattering which was recently carried out to next-to-next-to-leading order (NNLO) by Noam Shoresh and myself. In this calculation only potential pion contributions are included. These are the leading contributions from pions. A toy model was also considered in which potential pions are the only pion effects. The effective...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 1999