Abstract

Single-layer transition metal dichalcogenides are at the center of an ever increasing research effort both in terms of fundamental physics and applications. Exciton–phonon coupling plays a key role in determining the (opto)electronic properties of these materials. However, the exciton–phonon coupling strength has not been measured at room temperature. Here, we use two-dimensional micro-spectroscopy to determine exciton–phonon coupling of single-layer MoSe2. We detect beating signals as a function of waiting time induced by the coupling between A excitons and A′1 optical phonons. Analysis of beating maps combined with simulations provides the exciton–phonon coupling. We get a Huang–Rhys factor ~1, larger than in most other inorganic semiconductor nanostructures. Our technique offers a unique tool to measure exciton–phonon coupling also in other heterogeneous semiconducting systems, with a spatial resolution ~260 nm, and provides design-relevant parameters for the development of optoelectronic devices.

Highlights

  • Single-layer transition metal dichalcogenides are at the center of an ever increasing research effort both in terms of fundamental physics and applications

  • The reduced dimensionality is responsible for high exciton binding energies[7,8], making 1L-TMDs excellent candidates for optoelectronic devices at room temperature (RT)[2]

  • The presence of Exciton–phonon coupling (EXPC) was inferred from resonant Raman scattering[18,19], as well as time-resolved transmission measurements[20,21], where the A′1 optical phonon mode was observed to couple with the A excitonic resonance

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Summary

Introduction

Single-layer transition metal dichalcogenides are at the center of an ever increasing research effort both in terms of fundamental physics and applications. The presence of EXPC was inferred from resonant Raman scattering[18,19], as well as time-resolved transmission measurements[20,21], where the A′1 optical phonon mode was observed to couple with the A excitonic resonance.

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