Chinese Optics Letters, Volume. 23, Issue 1, 011901(2025)

Dispersions of two-photon and three-photon absorption in GaS films from 540 to 1600 nm

Yijie Wang, Jinhong Liu, Yanqing Ge, Erkang Li, Lili Zhao, Chunhui Lu*, Yixuan Zhou**, and Xinlong Xu***
Author Affiliations
  • Shaanxi Joint Laboratory of Graphene, State Key Laboratory Incubation Base of Photoelectric Technology and Functional Materials, International Collaborative Center on Photoelectric Technology and Nano Functional Materials, Institute of Photonics & Photon-Technology, School of Physics, Northwest University, Xi’an 710069, China
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    Figures & Tables(6)
    (a) SEM image, (b) Raman spectrum with an excitation wavelength of 532 nm, (c) XRD pattern, and (d) linear absorption spectrum and Tauc plot of the synthesized GaS film.
    (a) Open aperture Z-scan traces of the GaS film with excitation wavelengths of 540, 580, 620, 660, 800, 940, and 1040 nm at a pump intensity of about 200 GW/cm2. (b) The plots of ln (1−T) versus ln (I) to validate the order of nonlinearity, with solid lines representing the theoretical fitting.
    (a) Two-level system used to model the 2PA process. (b) Dispersion of 2PA coefficients as a function of Ephoton/Eg for GaS films, with solid lines representing theoretical fitting. (c) Normalized transmittance as a function of laser intensity under excitation wavelengths ranging from 540 to 1040 nm. (d) The fitted σ2PA parameters based on the two-level system.
    (a) Open aperture Z-scan traces of the GaS film under the excitation wavelengths from 1200 to 1600 nm at the pump intensity of about 60 GW/cm2. (b) The ln (1−T) as a function of ln(I). The solid lines represent the theoretical fitting.
    (a) Two-level system used for fitting the 3PA process. (b) Dispersion of 3PA coefficients as a function of Ephoton/Eg for GaS films, with solid lines representing theoretical fitting. (c) Normalized transmittance as a function of laser intensity under excitation wavelengths ranging from 1200 to 1600 nm. (d) The fitted σ3PA parameters based on the two-level system.
    • Table 1. The Summary of 2PA and 3PA Coefficients as Reported in the Literature

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      Table 1. The Summary of 2PA and 3PA Coefficients as Reported in the Literature

      MaterialLaser sourceβ2 (cm/GW)β3 (cm3/GW2)Ref.
      β-Ga2O3350 nm, 190 fs1.8[19]
      570 nm, 190 fs3.7 × 10−4[4]
      750 nm, 190 fs0.8 × 10−4
      β-GaS650 nm, 190 fs4900[12]
      GaN500 nm, 190 fs6.2[7]
      532 nm, 18 fs8.5
      860 nm, 190 fs1.8 × 10−3
      1000 nm, 190 fs3.5 × 10−3
      ZnO650 nm, 150 fs∼1[5]
      860 nm, 150 fs∼2 × 10−3
      ZnS780 nm, 120 fs0.024[6]
      MoS21300 nm, 150 fs2.2[24]
      (C4H9NH3)2PbBr41030 nm, 110 fs∼2[25]
      GaS620 nm, 60 fs19.89this work
      1500 nm, 52 fs4.88
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    Yijie Wang, Jinhong Liu, Yanqing Ge, Erkang Li, Lili Zhao, Chunhui Lu, Yixuan Zhou, Xinlong Xu, "Dispersions of two-photon and three-photon absorption in GaS films from 540 to 1600 nm," Chin. Opt. Lett. 23, 011901 (2025)

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    Paper Information

    Category: Nonlinear Optics

    Received: Jun. 22, 2024

    Accepted: Jul. 26, 2024

    Published Online: Feb. 10, 2025

    The Author Email: Chunhui Lu (luchunhui@nwu.edu.cn), Yixuan Zhou (yxzhou@nwu.edu.cn), Xinlong Xu (xlxuphy@nwu.edu.cn)

    DOI:10.3788/COL202523.011901

    CSTR:32184.14.COL202523.011901

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