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有限温度下捕获费米气体的动能

Kinetic Energy of a Trapped Fermi Gas at Finite Temperature.

作者信息

Grela Jacek, Majumdar Satya N, Schehr Grégory

机构信息

LPTMS, CNRS, Université Paris-Sud, Université Paris-Saclay, 91405 Orsay, France.

M. Smoluchowski Institute of Physics and Mark Kac Complex Systems Research Centre, Jagiellonian University, PL-30-059 Cracow, Poland.

出版信息

Phys Rev Lett. 2017 Sep 29;119(13):130601. doi: 10.1103/PhysRevLett.119.130601. Epub 2017 Sep 26.

Abstract

We study the statistics of the kinetic (or, equivalently, potential) energy for N noninteracting fermions in a 1d harmonic trap of frequency ω at finite temperature T. Remarkably, we find an exact solution for the full distribution of the kinetic energy, at any temperature T and for any N, using a nontrivial mapping to an integrable Calogero-Moser-Sutherland model. As a function of temperature T and for large N, we identify (i) a quantum regime, for T∼ℏω, where quantum fluctuations dominate and (ii) a thermal regime, for T∼Nℏω, governed by thermal fluctuations. We show how the mean and the variance as well as the large deviation function associated with the distribution of the kinetic energy cross over from the quantum to the thermal regime as T increases.

摘要

我们研究了在频率为ω的一维谐振子势阱中,处于有限温度T的N个非相互作用费米子的动能(或者等效地,势能)统计。值得注意的是,通过将其映射到一个可积的卡洛杰罗 - 莫泽 - 萨瑟兰模型,我们找到了在任意温度T和任意N下动能全分布的精确解。作为温度T的函数以及在大N的情况下,我们确定了(i)一个量子区域,对于T∼ℏω,其中量子涨落占主导,以及(ii)一个热区域,对于T∼Nℏω,由热涨落主导。我们展示了随着T增加,与动能分布相关的均值、方差以及大偏差函数是如何从量子区域过渡到热区域的。

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