FREEZEOUT PARAMETERS AND DYNAMICAL NET-CHARGE FLUCTUATIONS AT NICA ENERGIES
• 2016
معلومات البحث
المؤلفون
M. Hanafy1,2∗ , A. N. Tawfik2,3 , L. I. Abou-Salem1 , A. G. Shalaby1 , A. Sorin4 , O. Rogachevsky4 , W. Scheinast4
الكلمات المفتاحية
Not Available
المجلة العلمية
Not Available
الناشر
the Joint Institute for Nuclear Research Dubna, 14-18 March 2016 PROCEEDINGS
المجلد
Not Available
العدد
Not Available
الصفحات
34
publication.type
International
رابط البحث
Open Link
المواد المرفقة
Not Available
الملخص
The dependencies of different particle ratios on the nucleus-nucleus center-of-mass energy,
which can be related to the chemical potential, are calculated by using hadron resonance gas
(HRG) and Ultra-relativistic Quantum Molecular Dynamic (UrQMD) models. For UrQMD
two different types of phase transitions are taken into consideration, namely crossover and
first order, while the HRG model implements fully statistical aspects in describing the
particle production and their correlations, especially in the hadron phase. The freezeout
parameters, temperature (T ) and baryon chemical potential (μ), are deduced by fitting
various particle ratios estimated from UrQMD with HRG calculations at 7.7, 11.5, 19.6,
62.4 GeV. The results agree with the parameters which are independently determined
from statistical fit of the measured particle ratios and the thermal-statistical approaches.
Furthermore, the net-charge fluctuations for K/π, p/π and K/p determined UrQMD, and
HRG are compared with the available STAR and NA49 measurements. The future NICA
facility covers a wide range of low beam energies. The excellent agreement justifies the
conclusion that both UrQMD and HRG are suitable approaches to explain both freezeout
parameters and the dynamical net-charge fluctuations.
which can be related to the chemical potential, are calculated by using hadron resonance gas
(HRG) and Ultra-relativistic Quantum Molecular Dynamic (UrQMD) models. For UrQMD
two different types of phase transitions are taken into consideration, namely crossover and
first order, while the HRG model implements fully statistical aspects in describing the
particle production and their correlations, especially in the hadron phase. The freezeout
parameters, temperature (T ) and baryon chemical potential (μ), are deduced by fitting
various particle ratios estimated from UrQMD with HRG calculations at 7.7, 11.5, 19.6,
62.4 GeV. The results agree with the parameters which are independently determined
from statistical fit of the measured particle ratios and the thermal-statistical approaches.
Furthermore, the net-charge fluctuations for K/π, p/π and K/p determined UrQMD, and
HRG are compared with the available STAR and NA49 measurements. The future NICA
facility covers a wide range of low beam energies. The excellent agreement justifies the
conclusion that both UrQMD and HRG are suitable approaches to explain both freezeout
parameters and the dynamical net-charge fluctuations.
أعضاء هيئة التدريس - جامعة بنها