Vibrational cooling and thermoelectric response of nanoelectromechanical systems

TL;DR

This paper investigates phonon cooling in nanoelectromechanical systems using thermoelectric principles, demonstrating conditions under which efficiency approaches the Carnot limit, with analysis in quantum and classical regimes.

Contribution

It extends thermoelectric theory to phonon cooling in nanoelectromechanical systems and analyzes a realistic double-quantum-dot model for efficiency and temperature control.

Findings

Efficiency can approach Carnot limit in the quantum regime.

Large figures of merit are achievable in the quantum regime.

Efficiency is generally far from Carnot in the classical regime.

Abstract

An important goal in nanoelectromechanics is to cool the vibrational motion, ideally to its quantum ground state. Cooling by an applied charge current is a particularly simple and hence attractive strategy to this effect. Here, we explore this phenomenon in the context of the general theory of thermoelectrics. In linear response, this theory describes thermoelectric refrigerators in terms of their cooling efficiency and figure of merit ZT. We show that both concepts carry over to phonon cooling in nanoelectromechanical systems. As an important consequence, this allows us to discuss the efficiency of phonon refrigerators in relation to the fundamental Carnot efficiency. We illustrate these general concepts by thoroughly investigating a simple double-quantum-dot model with the dual advantage of being quite realistic experimentally and amenable to a largely analytical analysis theoretically. Specifically, we obtain results for the efficiency, the figure of merit, and the effective temperature of the vibrational motion in two regimes. In the quantum regime in which the vibrational motion is fast compared to the electronic degrees of freedom, we can describe the electronic and phononic dynamics of the model in terms of master equations. In the complementary classical regime of slow vibrational motion, the dynamics is described in terms of an appropriate Langevin equation. Remarkably, we find that the efficiency can approach the maximal Carnot value in the quantum regime, with large associated figures of merit. In contrast, the efficiencies are typically far from the Carnot limit in the classical regime. Our theoretical results should provide guidance to implementing efficient vibrational cooling of nanoelectromechanical systems in the laboratory.