Abstract

Long wavelength polar vibrations in monolayer (ML) transition metal dichalcogenides (TMDs) are systematically studied for in-plane and out-of-plane motions, using two pairs of macroscopic equations deduced from a microscopic dipole lattice model accounting for local field effects (LFEs) and electronic polarization (EP). Longitudinal and transverse optical modes and out-of-plane modes are derived, and the analytical expressions describe previous first-principles calculations very well. Owing to the LFEs, the in-plane dielectric susceptibilities of ML TMDs are one order of magnitude greater than the out-of-plane susceptibilities. Furthermore, the effects of the dielectric environment on the polar vibrations are studied. Both EP and LFEs should be accounted for obtaining an accurate evaluation of dielectric susceptibility and key lattice-dynamical properties such as Born charge and phonon dispersion. A two-dimensional (2D) Lyddane–Sachs–Teller relation and a frequency–susceptibility relation are derived for in-plane and out-of-plane motions, relating the 2D dielectric functions or susceptibilities to the polar phonon frequencies. The results are also compared in detail with those of ML hexagonal boron nitride.

Highlights

  • Monolayer (ML) transition metal dichalcogenides (TMDs) such as MoS2 are two-dimensional (2D) polar crystals in which the polar lattice vibrations occur together with the nonpolar vibrations

  • We have studied long wavelength optical vibrations in ML TMDs using the macroscopic equations (MEs) deduced from a microscopic dipole lattice model, including electronic polarization (EP) and local field effects (LFEs) self-consistently

  • The longitudinal optical (LO) mode dispersion relation is identical to the analytical expression of Sohier et al A 2D LST relation and a frequency–susceptibility relation are derived for in-plane and out-of-plane vibrations, respectively, relating the 2D dielectric functions or susceptibilities to the polar mode frequencies

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Summary

Introduction

Monolayer (ML) transition metal dichalcogenides (TMDs) such as MoS2 are two-dimensional (2D) polar crystals in which the polar lattice vibrations occur together with the nonpolar vibrations. With one transition-metal ion and two same chalcogen ions per cell, the ML TMD has three branches of polar optical modes due to the contrary motions of the chalcogen and metal ions, as well as three branches of nonpolar optical modes corresponding to the relative motions of the two chalcogen ions. These optical branches are composed of the in-plane nonpolar LO and transverse optical (TO) modes (labeled LO1, TO1) and polar LO and TO modes (labeled LO2, TO2), and the out-of-plane nonpolar modes ZO2 and polar modes ZO1.17,18

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