Abstract

The tunability of the interlayer coupling by twisting one layer with respect to another layer of two-dimensional materials provides a unique way to manipulate the phonons and related properties. We refer to this engineering of phononic properties as "Twistnonics". We study the effects of twisting on low-frequency shear (SM) and layer breathing (LBM) modes in transition metal dichalcogenide (TMD) bilayer using atomistic classical simulations. We show that these low-frequency modes are extremely sensitive to twist and can be used to infer the twist angle. We find unique "ultra-soft" phason modes (frequency $\lesssim 1\ \mathrm{cm^{-1}}$, comparable to acoustic modes) for any non-zero twist, corresponding to an \textit{effective} translation of the moir{\'e} lattice by relative displacement of the constituent layers in a non-trivial way. Unlike the acoustic modes, the velocity of the phason modes is quite sensitive to twist angle. As twist angle decreases, ($\theta \lesssim 3^{\circ},\ \gtrsim 57^{\circ}$) the ultra-soft modes represent the acoustic modes of the "emergent" soft moir{\'e} scale lattice. Also, new high-frequency SMs appear, identical to those in stable bilayer TMD ($\theta = 0\degree/60\degree$), due to the overwhelming growth of stable stacking regions in relaxed twisted structures. Furthermore, we find remarkably different structural relaxation as $\theta \to 0^{\circ}$, $\to 60^{\circ}$ due to sub-lattice symmetry breaking. Our study reveals the possibility of an intriguing $\theta$ dependent superlubric to pinning behavior and of the existence of ultra-soft modes in \textit{all} two-dimensional (2D) materials.

Highlights

  • Twisting one layer of a bilayer system with respect to another provides a unique degree of freedom for tuning the properties of two-dimensional (2D) materials

  • In this work we computationally investigate the effects of twisting on low-frequency shear modes (SMs) and layer breathing modes (LBMs) in bilayer MoS2, a prototypical transition-metal dichalcogenide (TMD)

  • We have shown that the low-frequency modes are extremely sensitive to twisting in the twisted TMD bilayer and can be used as a probe to determine the twist angle

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Summary

Introduction

Twisting one layer of a bilayer system with respect to another provides a unique degree of freedom for tuning the properties of two-dimensional (2D) materials. An important facet of twisting is the evolution of low-frequency vibrational modes, which has largely remained unexplored. Since the low-frequency modes are solely determined by interlayer coupling and are accessible in Raman measurements, they provide a direct nondestructive probe of the interlayer interaction [27,28,29,30]. The existing theoretical reports on the evolution of vibrational modes in twisted structures are restricted to large twist angles and use the Lennard-Jones potential [31] to describe the interlayer interaction, which is insufficient for capturing the stackingdependent energetics [32]. Existing experimental studies [29,30,33] have explored small twist angles, they can only probe Raman active modes with frequencies greater than 10 cm−1

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