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Dimensional crossover of thermal transport in quantum harmonic lattices coupled to self-consistent reservoirs.
Physical Review E ( IF 2.2 ) Pub Date : 2020-07-08 , DOI: 10.1103/physreve.102.012121 Kiminori Hattori 1 , Masaya Sambonchiku 1
Physical Review E ( IF 2.2 ) Pub Date : 2020-07-08 , DOI: 10.1103/physreve.102.012121 Kiminori Hattori 1 , Masaya Sambonchiku 1
Affiliation
In this study, we investigate thermal transport in -dimensional quantum harmonic lattices coupled to self-consistent reservoirs. The -dimensional system is treated as a set of Klein-Gordon chains by exploiting an orthogonal transformation. For generality, the self-energy that describes the reservoir-system coupling is assumed to be a power function of energy , where is limited to odd integers because of the reality condition. Total momentum conservation is violated for but otherwise preserved. In this approach, we show that for , thermal conductivity remains finite in the thermodynamic limit and normal transport takes place for an arbitrary value of . For , however, thermal conductivity diverges and thermal transport becomes anomalous as long as , whereas normal transport is recovered when . These criteria derived for quantum-mechanical lattices imply that normal transport emerges in high enough dimensions despite total momentum conservation and reinforce the prevailing conjecture deduced in the classical limit.
中文翻译:
耦合到自洽储层的量子谐波晶格中热输运的尺寸跨度。
在这项研究中,我们调查了 维自洽储层的三维量子谐波晶格。的通过利用正交变换将三维系统视为一组Klein-Gordon链。一般而言,描述储层与系统耦合的自能量被假定为能量的幂函数。,在哪里 由于现实情况,仅限于奇数整数。违反了总动量守恒但保留下来。通过这种方法,我们证明了,热导率在热力学极限内保持有限,并且在任意值的情况下发生正常传输 。对于但是,只要热导率发生变化,热传递就会变得异常 ,而当 。这些为量子力学晶格推导的标准表明,尽管总动量守恒,法向输运仍以足够高的尺寸出现,并加强了经典极限中的普遍猜想。
更新日期:2020-07-08
中文翻译:
耦合到自洽储层的量子谐波晶格中热输运的尺寸跨度。
在这项研究中,我们调查了 维自洽储层的三维量子谐波晶格。的通过利用正交变换将三维系统视为一组Klein-Gordon链。一般而言,描述储层与系统耦合的自能量被假定为能量的幂函数。,在哪里 由于现实情况,仅限于奇数整数。违反了总动量守恒但保留下来。通过这种方法,我们证明了,热导率在热力学极限内保持有限,并且在任意值的情况下发生正常传输 。对于但是,只要热导率发生变化,热传递就会变得异常 ,而当 。这些为量子力学晶格推导的标准表明,尽管总动量守恒,法向输运仍以足够高的尺寸出现,并加强了经典极限中的普遍猜想。