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arXiv 0811.2078cond-mat.stat-mechcond-mat.mes-hall
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正常介观费米子系统的正则heat capacity:温度演化和粒子数振荡

The canonical heat capacity of normal mesoscopic fermion systems: the temperature evolution and particle number oscillations

N. K. Kuzmenko, V. M. Mikhajlov

摘要:

本文研究了作为独立粒子正则系综的介观非超导费米子系统在粒子数和温度从接近于零到费米能的范围内的热容(C)。C的温度演化自然分为四个阶段。在第一个热容量随温度呈指数增加,并在共振温度达到局部最大值或不规则的增长。测量的共振温度可以给出费米能附近能级间距的信息。在第二阶段,发生能级密度振荡的逐步抑制。在这个阶段,C与S的振荡。可以清楚地观察到粒子数N。这些振荡给出了温度平均能级密度的N-变化。当粒子数足够大(N>1000)时,C在第三阶段的增长服从T-线性规律。结果表明,与C与N严格成正比的大系统相比,这种小系统线性律中的索末菲因子表现出更复杂的N依赖性。当温度趋向于费米能时,偏离T线性是明显的,当T大于费米能时(演化的第四阶段),任何系统都达到经典的玻尔兹曼-麦克斯韦极限,而与粒子无关。

英文摘要:

The heat capacity (C) of a mesoscopic nonsuperconducting fermion system treated as a canonical ensemble of independent particles is studied in a wide range of particle numbers and temperatures which vary from values close to zero up to the Fermi energy. The temperature evolution of C is naturally divided into four stages. On the first one the heat capacity exponentially increases with temperature and at a resonance temperature reaches either a local maximum or an irregularity in its growth. This resonance temperature being measured can give information concerning the level spacings in the immediate proximity of the Fermi energy. On the second stage the progressive suppression of the level density oscillations takes place. During this stage oscillations of C v.s. particle number N can be distinctly observed. These oscillations give the N-variations of the temperature averaged level density. The growth of C on the third stage of the evolution is governed by the T-linear law if the particle number is large enough (N>1000). It is found that the Sommerfeld factor in the linear law for such small systems shows more complicated N-dependence as compared with large systems where C is strictly proportional to N. For temperatures tending to the Fermi energy the deviations from the T-linearity are evident and at T larger than the Fermi energy (the fourth stage of the evolution) any system attains to the classic Boltzmann-Maxwell limit irrespective of the particle

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