Density and temperature of fermions and bosons from quantum fluctuations

被引:0
作者
Zheng Hua [1 ,2 ]
Giuliani, Gianluca [1 ]
Bonasera, Aldo [1 ,3 ]
机构
[1] Texas A&M Univ, Inst Cyclotron, College Stn, TX 77843 USA
[2] Texas A&M Univ, Dept Phys & Astron, College Stn, TX 77843 USA
[3] Ist Nazl Fis Nucl, Lab Nazl Sud, I-95123 Catania, Italy
关键词
Density; Temperature; Fermions; Bosons; Quantum fluctuations; Bose-Einstein condensate; NUCLEAR; COLLISIONS; DYNAMICS; EQUATION; SYSTEMS; STATE;
D O I
暂无
中图分类号
TL [原子能技术]; O571 [原子核物理学];
学科分类号
0827 ; 082701 ;
摘要
A novel method to determine the density and temperature of a system constituted by fermions and/or bosons is proposed based on quantum fluctuations. For fermions system, the results in the limit where the reached temperature T is small and where there is no constraint for the reached temperature T compared to the Fermi energy epsilon(f) at a given density rho are given, respectively. Quadrupole and multiplicity fluctuation relations are derived in terms of T/epsilon(f). We compared the two set results in the limit when T is much smaller compared to Fermi energy epsilon(f) and they are consistent, as expected. The classical limit is also obtained for high temperatures and low densities. For bosons system, quadrupole and multiplicity fluctuations using Landau's theory of fluctuations near the critical point for a Bose-Einstein condensate (BEC) at a given density rho are derived. As an example, we apply our approach to heavy ion collisions using the Constrained Molecular Dynamics model (CoMD) which includes the fermionic statistics. The multiplicity fluctuation quenching for fermions is found in the model and confirmed by experimental data. To reproduce the available experimental data better, we propose a modification of the collision term in the approach to include the possibility of alpha-alpha collisions. The relevant Bose-Einstein factor in the collision term is properly taken into account. This approach increases the yields of bosons relative to fermions closer to data. Boson fluctuations become larger than one as expected.
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