Sound waves and flexural mode dynamics in two-dimensional crystals

K. H. Michel, P. Scuracchio, and F. M. Peeters
Phys. Rev. B 96, 094302 – Published 5 September 2017

Abstract

Starting from a Hamiltonian with anharmonic coupling between in-plane acoustic displacements and out-of-plane (flexural) modes, we derived coupled equations of motion for in-plane displacements correlations and flexural mode density fluctuations. Linear response theory and time-dependent thermal Green's functions techniques are applied in order to obtain different response functions. As external perturbations we allow for stresses and thermal heat sources. The displacement correlations are described by a Dyson equation where the flexural density distribution enters as an additional perturbation. The flexural density distribution satisfies a kinetic equation where the in-plane lattice displacements act as a perturbation. In the hydrodynamic limit this system of coupled equations is at the basis of a unified description of elastic and thermal phenomena, such as isothermal versus adiabatic sound motion and thermal conductivity versus second sound. The general theory is formulated in view of application to graphene, two-dimensional h-BN, and 2H-transition metal dichalcogenides and oxides.

  • Figure
  • Received 24 May 2017
  • Revised 17 August 2017

DOI:https://doi.org/10.1103/PhysRevB.96.094302

©2017 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied PhysicsStatistical Physics & Thermodynamics

Authors & Affiliations

K. H. Michel*, P. Scuracchio, and F. M. Peeters

  • Universiteit Antwerpen, Department of Physics, Groenenborgerlaan 171, Be-2020 Antwerpen, Belgium

  • *ktdm@skynet.be
  • pablo.scuracchio@uantwerpen.be
  • francois.peeters@uantwerpen.be

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Issue

Vol. 96, Iss. 9 — 1 September 2017

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