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On spatially homogeneous solutions of a modified Boltzmann equation for Fermi-Dirac particles

机译:关于费米-狄拉克粒子的修正玻耳兹曼方程的空间齐次解

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The paper considers a modified spatially homogeneous Boltzmann equation for Fermi Dirac particles (BFD). We prove that for the BFD equation there are only two classes of equilibria: the first ones are Fermi Dirac distributions, the second ones are characteristic functions of the Euclidean balls, and they can be simply classified in terms of temperatures: T > 2/5 T-F and T = 2/5 T-F, where T-F denotes the Fermi temperature. In general we show that the L-infinity-bound 0 less than or equal to f less than or equal to 1/epsilon derived from the equation for solutions implies the temperature inequality T greater than or equal to 2/5 T-F and if T > 2/5 T-F, then f trend towards Fermi Dirac distributions; if T = 2/5 T-F, then f are the second equilibria. In order to study the long-time behavior, we also prove the conservation of energy and the entropy identity, and establish the moment production estimates for hard potentials. [References: 22]
机译:本文考虑了费米·狄拉克粒子(BFD)的修正空间齐次Boltzmann方程。我们证明,对于BFD方程,只有两类平衡:第一类是费米·狄拉克分布,第二类是欧几里得球的特征函数,可以简单地根据温度对其进行分类:T> 2/5 TF和T = 2/5 TF,其中TF表示费米温度。通常,我们表明,从溶液方程导出的L无限边界0小于或等于f小于/等于1 /ε表示温度不等式T大于或等于2/5 TF,并且如果T> 2/5 TF,然后是Fermi Dirac分布的f趋势;如果T = 2/5 T-F,则f是第二个平衡点。为了研究长期行为,我们还证明了能量守恒和熵恒等式,并为硬势建立了瞬时产量估计。 [参考:22]

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