Time-dependent quantum transport and power-law decay of the transient current in a nano-relay and nano-oscillator

TL;DR

This paper uses nonequilibrium Green's functions to analyze transient electron transport in nano-devices, revealing power-law decay of current and complex dynamical behaviors influenced by bias and coupling parameters.

Contribution

It provides a numerically exact expression for transient current and uncovers the power-law decay and non-trivial maximum current timing in nano-circuits with time-dependent couplings.

Findings

Transient current overshoots and oscillates before settling.

Power-law decay of current depends on bias and coupling.

Maximum current timing is influenced by device parameters.

Abstract

Time-dependent nonequilibrium Green's functions are used to study electron transport properties in a device consisting of two linear chain leads and a time-dependent interleads coupling that is switched on non-adiabatically. We derive a numerically exact expression for the particle current and examine its characteristics as it evolves in time from the transient regime to the long-time steady-state regime. We find that just after switch-on the current initially overshoots the expected long-time steady-state value, oscillates and decays as a power law, and eventually settles to a steady-state value consistent with the value calculated using the Landauer formula. The power-law parameters depend on the values of the applied bias voltage, the strength of the couplings, and the speed of the switch-on. In particular, the oscillating transient current decays away longer for lower bias voltages. Furthermore, the power-law decay nature of the current suggests an equivalent series resistor-inductor-capacitor circuit wherein all of the components have time-dependent properties. Such dynamical resistive, inductive, and capacitive influences are generic in nano-circuites where dynamical switches are incorporated. We also examine the characteristics of the dynamical current in a nano-oscillator modeled by introducing a sinusoidally modulated interleads coupling between the two leads. We find that the current does not strictly follow the sinusoidal form of the coupling. In particular, the maximum current does not occur during times when the leads are exactly aligned. Instead, the times when the maximum current occurs depend on the values of the bias potential, nearest-neighbor coupling, and the interleads coupling.