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    Raman spectra evolution in γ-, ε-, and β-InSe: Stacking-dependent phonons and analytical lattice dynamics

    Bingye Chen*, Weifeng Huang*, Bin Jiang, 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

    • *These authors contributed equally to this work.
    • †Contact author: luox77@mail.sysu.edu.cn

    Phys. Rev. B 114, 185406 – Published 3 September, 2026

    DOI: https://doi.org/10.1103/26rq-4m96

    Abstract

    Stacking order and layer thickness exert significant influence on the physical properties of two-dimensional materials. Here, using first-principles calculations and symmetry analysis, we theoretically investigate the stacking- and layer-dependent Raman responses of InSe and infer the corresponding symmetry-based second-harmonic generation (SHG) selection rules. For bulklike InSe, the calculated low-frequency Raman spectra (below 30 cm−1) enable direct phase-sensitive spectral fingerprints: no peak is found for γ-InSe, whereas ε- and β-InSe exhibit peaks near 20.2 and 17.8 cm−1, respectively. Point-group analysis further indicates that SHG response is symmetry-allowed for bulk γ- and ε-InSe, whereas it is symmetry-forbidden for bulk β-InSe. For few-layer InSe, the frequencies of the strongest shear modes exhibit a blueshift for the AB-stacked ε and β phases, but a redshift for the ABC-stacked γ phase, as the layer number increases. SHG response is symmetry-allowed for both odd- and even-layer γ- and ε-InSe, whereas it is allowed for odd layers and forbidden for even layers in β phase. This layer-dependent evolution of the low-frequency Raman modes, combined with symmetry-based SHG selection rules, provide an effective route for distinguishing the three InSe polytypes in the few-layer regime. In the high-frequency region, the A′11(∼110 cm−1) and A′12(∼235 cm−1) modes display a blueshift and a redshift, respectively, for all three phases with increasing layer thickness. The low-frequency shear modes and the frequency difference between A′11 and A′12 can serve as indicators of layer number in ultrathin films. Combined with analytical lattice-dynamical models, we reveal that the competition between the surface effect and the thickness effect governs the overall evolution of the high-frequency Raman trends. This work clarifies the microscopic origin of Raman responses in InSe and provides theoretical guidance for phase identification, thickness estimation, and elastic modulus characterization of layered materials.

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