Phonon Bandgap Engineering of Strained Monolayer MoS2

Abstract

The phonon band structure of monolayer MoS2 is characteristic for a large energy gap between acoustic and optical branches, which protects the vibration of acoustic modes from being scattered by optical phonon modes. Therefore, the phonon bandgap engineering is of practical significance for the manipulation of phonon-related mechanical or thermal properties in monolayer MoS2. We perform both phonon analysis and molecular dynamics simulations to investigate the tension effect on the phonon bandgap and the compression induced instability of the monolayer MoS2. Our key finding is that the phonon bandgap can be narrowed by the uniaxial tension, and is completely closed at epsilon=0.145; while the biaxial tension only has limited effect on the phonon bandgap. We also demonstrate the compression induced buckling for the monolayer MoS2. The critical strain for buckling is extracted from the band structure analysis of the flexure mode in the monolayer MoS2 and is further verified by molecular dynamics simulations and the Euler buckling theory. Our study illustrates the uniaxial tension as an efficient method for manipulating the phonon bandgap of the monolayer MoS2, while the biaxial compression as a powerful tool to intrigue buckling in the monolayer MoS2.

Nanoscale, published

References in corpus (5)

• Emerging Device Applications for Semiconducting Two-Dimensional Transition Metal Dichalcogenides
• Uniaxial Strain in Graphene by Raman Spectroscopy: G peak splitting, Gruneisen Parameters and Sample Orientation
• All-graphene integrated circuits via strain engineering
• MoS2 Nanoresonators: Intrinsically Better Than Graphene?
• Strain induced conductance modulation in graphene grain boundary

Cited by in corpus (4)

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• Graphene Versus MoS2: a Short Review
• A Review on Flexural Mode of Graphene: Lattice Dynamics, Thermal Conduction, Thermal Expansion, Elasticity, and Nanomechanical Resonance
• Rigid Unit Modes in $sp$-$s{p}^2$ Hybridized Carbon Systems: Origin of Negative Thermal Expansion