Layer-selective Optical Second-harmonic Generation Spectroscopy of a MoS<sub>2</sub>/WSe<sub>2</sub> Heterobilayer

The so-called C exciton resonance enhancement peak for heterostructures (HSs) of transition-metal dichalcogenides is indicative of a change in the band structure due to interlayer coupling. However, the superposition of the broad C exciton peaks from the two layers presents a significant challenge to the analysis of the alteration. The aim of this study was to gain insight into the electronic states of the C exciton region in each layer of a MoS2/WSe2 HS. To this end, we obtained second-harmonic generation (SHG) spectra of the HS by fixing the incident polarization angle to sequentially minimize the second-harmonic signals from the WSe2 and MoS2 layers. The resulting SHG spectra comprised signals from the MoS2 (former case) and WSe2 layers (latter case), demonstrating that the C exciton peak from each layer of the HS could be observed individually.

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Publication Details

Journal
e-Journal of Surface Science and Nanotechnology
Published
2025-03-07
DOI
https://doi.org/10.1380/ejssnt.2025-013
Primary Topic
Spectroscopy and Quantum Chemical Studies
Type
article
Field-Weighted Citation Impact
0.00

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article

Layer-selective Optical Second-harmonic Generation Spectroscopy of a MoS2/WSe2 Heterobilayer

S. Ohno, Yasuyuki Hirata, Yoshihiro Miyauchi
4 links
e-Journal of Surface Science and Nanotechnology
Spectroscopy and Quantum Chemical Studies
article

Layer-selective Optical Second-harmonic Generation Spectroscopy of a MoS2/WSe2 Heterobilayer

S. Ohno, Yasuyuki Hirata, Yoshihiro Miyauchi
article en

Abstract

The so-called C exciton resonance enhancement peak for heterostructures (HSs) of transition-metal dichalcogenides is indicative of a change in the band structure due to interlayer coupling. However, the superposition of the broad C exciton peaks from the two layers presents a significant challenge to the analysis of the alteration. The aim of this study was to gain insight into the electronic states of the C exciton region in each layer of a MoS2/WSe2 HS. To this end, we obtained second-harmonic generation (SHG) spectra of the HS by fixing the incident polarization angle to sequentially minimize the second-harmonic signals from the WSe2 and MoS2 layers. The resulting SHG spectra comprised signals from the MoS2 (former case) and WSe2 layers (latter case), demonstrating that the C exciton peak from each layer of the HS could be observed individually.

e-Journal of Surface Science and NanotechnologyVol. 23(1)
Yokohama National University (JP), National Defense Academy of Japan (JP)
Japan Society for the Promotion of Science
Openalex Percentile: Top 97%
Spectroscopy and Quantum Chemical Studies
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