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PION-PAIR FORMATION AND THE PION DISPERSION RELATION IN A HOT PION GAS

机译:热离子气中的离子对形成和离子弥散关系

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摘要

The possibility of pion-pair formation in a hot pion gas, based on the bosonic gap equation, is pointed out and discussed in detail. The critical temperature for condensation of pion pairs (Evans-Rashid transition) is determined as a function of the pion density. As for fermions, this phase transition is signaled by the appearance of a pole in the two-particle propagator, In Bose systems there exists a second, lower critical temperature, associated with the appearance of the single-particle condensate. Between the two critical temperatures the pion dispersion relation changes from the usual quasiparticle dispersion to a Bogoliubov-like dispersion relation at low momenta. This generalizes the non-relativistic result for an attractive Bose gas by Evans et al. Possible consequences for the inclusive pion spectra measured in heavy-ion collisions at ultra-relativistic energies are discussed. [References: 21]
机译:指出并详细讨论了基于玻色子间隙方程的热介子气中形成偶子对的可能性。确定离子对凝结的临界温度(Evans-Rashid跃迁)作为离子浓度的函数。至于费米子,这种相变是通过两粒子传播器中的一个极点出现来表示的。在Bose系统中,存在一个较低的第二临界温度,与单粒子冷凝物的出现有关。在两个临界温度之间,介电子弥散关系从通常的准粒子弥散关系变为低动量的类似于Bogoliubov的弥散关系。这概括了Evans等人对有吸引力的Bose气体的非相对论性结果。讨论了在超相对论能量下重离子碰撞中测得的包容性离子光谱的可能结果。 [参考:21]

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