Enhancing phonon flow through 1D interfaces by Impedance Matching

TL;DR

This paper applies impedance matching principles from microwave engineering to optimize phonon transmission at 1D interfaces, enhancing thermal conductance through tailored contact properties and graded junctions.

Contribution

It introduces a generalized impedance matching framework for phonons using contact broadening matrices, proposing optimal conductance criteria and graded interface designs for improved thermal transport.

Findings

Optimal conductance occurs when contact broadening equals the geometric mean.

Matching low-frequency impedance minimizes interfacial resistance.

Graded junctions with exponential broadening improve broadband phonon transmission.

Abstract

We extend concepts from microwave engineering to thermal interfaces and explore the principles of impedance matching in 1D. The extension is based on the generalization of acoustic impedance to non linear dispersions using the contact broadening matrix $\Gamma(\omega)$, extracted from the phonon self energy. For a single junction, we find that for coherent and incoherent phonons the optimal thermal conductance occurs when the matching $\Gamma(\omega)$ equals the Geometric Mean (GM) of the contact broadenings. This criteria favors the transmission of both low and high frequency phonons by requiring that (1) the low frequency acoustic impedance of the junction matches that of the two contacts by minimizing the sum of interfacial resistances; and (2) the cut-off frequency is near the minimum of the two contacts, thereby reducing the spillage of the states into the tunneling regime. For an ultimately scaled single atom/spring junction, the matching criteria transforms to the arithmetic mean for mass and the harmonic mean for spring constant. The matching can be further improved using a composite graded junction with an exponential varying broadening that functions like a broadband antireflection coating. There is however a trade off as the increased length of the interface brings in additional intrinsic sources of scattering.