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    Pathway- and momentum-resolved resonance Raman scattering in monolayer and bilayer InSe

    Bingye Chen, Xin Luo*, and Yue Zheng†

    • Guangdong Provincial Key Laboratory of Magnetoelectric Physics and Devices, School of Physics, Sun Yat-sen University, Guangzhou 510275, China; State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, Sun Yat-sen University, Guangzhou 510275, China; and Interdisciplinary Research Centre for Physical Mechanics in Complex Systems and Its Engineering Applications, School of Physics, Sun Yat-sen University, Guangzhou 510275, China

    • *Contact author: luox77@mail.sysu.edu.cn
    • †Contact author: zhengy35@mail.sysu.edu.cn

    Phys. Rev. B 114, 185305 – Published 21 September, 2026

    DOI: https://doi.org/10.1103/8hv7-ls9p

    Abstract

    Resonance Raman spectroscopy is a powerful tool for probing electron–phonon coupling, phonon momentum distributions, and stacking-related spectral features in InSe. Based on first-principles calculations, we systematically investigate the single-resonance Raman (SRR) and double-resonance Raman (DRR) scattering behaviors of monolayer InSe and bilayer β- and ε-phase InSe. For monolayer InSe, the SRR response is dominated by the hole-scattering pathway (h-path), while the out-of-plane, out-of-phase Se–In vibration near 235cm−1 (A1′2) exhibits the strongest resonance enhancement. The principal DRR peaks mainly originate from near-Γ intravalley overtone scattering of the in-plane Se–In relative-vibration branch (E′2) and exhibit weak excitation-energy dispersion, while the mixed electron–hole scattering pathways (eh- and he-paths) also make appreciable contributions. Under 4.66eV excitation, the high-frequency broad band evolves into two components, associated with additional strong resonant optical-transition channels along the Σ–M direction. For bilayer InSe, the resonance enhancement of low-frequency interlayer phonon modes in the SRR spectra provides fingerprints of the layer number. In the DRR spectra, the nearly excitation-energy-independent lower-frequency principal peak (P1) is blue-shifted by approximately 9cm−1 relative to monolayer InSe and can serve as a layer-number indicator, whereas the broad higher-frequency peak (P3) is more sensitive to stacking order and excitation energy, with the ε phase expected to exhibit a more pronounced excitation-energy-induced shift than the β phase. These results clarify the microscopic origin of resonance Raman scattering in InSe and provide a theoretical basis for characterizing its layer number, interlayer vibrations, and stacking structures.

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