论文标题

量子点系统的通用和热电运输特性

Universality and thermoelectric transport properties of quantum dot systems

论文作者

Aranguren-Quintero, D. F., Ramos, E., Silva-Valencia, J., Figueira, M. S., Oliveira, L. N., Franco, R.

论文摘要

我们讨论了与量子线相连的量子点的半导体纳米结构的温度依赖性热电传输特性:电导,导电电导和热电器的热依赖性。我们探讨了与近托跨界的温度范围内热电特性的普遍性。在此热范围内,一般参数表明,任何平衡属性的温度依赖性都应该是比率$ t^{*} = t/t_ {k} $的通用函数,其中$ t_ {k {k} $是近kondo温度。考虑到粒子 - 孔对称,自旋定位安德森模型,已经显示出零偏置电导能通过嵌入或侧耦合到量子线的量子点线性地映射到通用电导率上。我们采用严格的重新分配组参数,计算通用热电传输系数,使我们能够将此结果扩展到热电器和热电导率。我们提出了数值重归于组的结果,以说明我们发现的物理。将通用的热电系数应用于近托政权的不同温度下的电导电导和热压的最新实验结果,我们计算所有可用于预测这些属性实验结果的简单分析拟合功能。但是,由于缺乏广泛的温度范围内可用的实验结果,我们无法检查所有这些。

We discuss the temperature-dependent thermoelectric transport properties of semiconductor nanostructures comprising a quantum dot coupled to quantum wires: the thermal dependence of the electrical conductance, thermal conductance, and thermopower. We explore the universality of the thermoelectric properties in the temperature range associated with the Kondo crossover. In this thermal range, general arguments indicate that any equilibrium property's temperature dependence should be a universal function of the ratio $T^{*}=T/T_{K}$, where $T_{K}$ is the Kondo temperature. Considering the particle-hole symmetric, spin-degenerate Anderson model, the zero-bias electrical conductance has already been shown to map linearly onto a universal conductance through a quantum dot embedded or side-coupled to a quantum wire. Employing rigorous renormalization-group arguments, we calculate universal thermoelectric transport coefficients that allow us to extend this result to the thermopower and the thermal conductance. We present numerical renormalization-group results to illustrate the physics in our findings. Applying the universal thermoelectric coefficients to recent experimental results of the electrical conductance and thermo-voltages versus $V_{gate}$, at different temperatures in the Kondo regime, we calculate all the thermoelectric properties and obtain simple analytical fitting functions that can be used to predict the experimental results of these properties. However, we cannot check all of them, due to the lack of available experimental results over a broad temperature range.

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