Photonics Research, Volume. 9, Issue 5, 678(2021)

Principles to tailor the saturable and reverse saturable absorption of epsilon-near-zero material

Hao Ma1,2,3, Yuanan Zhao1,2,3、*, Yuchen Shao1,2,3, Yafei Lian1,2,3, Weili Zhang1,2,3, Guohang Hu1,2,3, Yuxin Leng4, and Jianda Shao1,2,3,5,6
Author Affiliations
  • 1Laboratory of Thin Film Optics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Key Laboratory of Materials for High Power Laser, Chinese Academy of Sciences, Shanghai 201800, China
  • 4State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 5Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou 310024, China
  • 6e-mail: jdshao@siom.ac.cn
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    Figures & Tables(9)
    Characterization of as-deposited and annealed ITO films. SEM images showing (a) as-deposited ITO film and (b) ITO film annealed at 400˚C. (c) X-ray diffraction pattern. (d) Linear optical transmittance spectrum.
    Real and imaginary components of the permittivity of ITO films. (a) As-deposited ITO film. (b) Post-annealed ITO film.
    Optical nonlinear absorption measurement setup based on the Z-scan method.
    Open aperture Z-scan results of as-deposited ITO films under excitation of 1030 nm at different input fluences.
    Open aperture Z-scan results of as-deposited ITO films under excitation of 1440 nm at different input fluences. (a) OA Z-scan. (b) CA Z-scan.
    Dependence of normalized transmittance of ITO films (as-deposited and annealed) on optical intensity using different pump sources. (a) 1030 nm. (b) 1440 nm.
    Transient response of Te and Tl obtained using the two-temperature model under different pump fluences. (a) 1030 nm excitation. (b) 1440 nm excitation.
    • Table 1. Saturated Absorption Intensity (Is) and Corresponding Three-Photon Absorption Coefficient (γ)

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      Table 1. Saturated Absorption Intensity (Is) and Corresponding Three-Photon Absorption Coefficient (γ)

      Laser Intensity (GW/cm2)24.561.291.8122.4214.2
      Is (GW/cm2)64.467.176.1105.988.5
      γ (cm3/GW2)3.6×1036.0×1034.9×1026.1×1028.8×102
    • Table 2. Hall-Effect Properties of As-deposited and Annealed ITO Films

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      Table 2. Hall-Effect Properties of As-deposited and Annealed ITO Films

      SamplesCarrier Concentration (cm3)Mobility [cm2/(V·s)]Resistivity (Ω·cm)
      As-deposited7.5×102131.52.2
      Annealed1.6×102139.711.9
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    Hao Ma, Yuanan Zhao, Yuchen Shao, Yafei Lian, Weili Zhang, Guohang Hu, Yuxin Leng, Jianda Shao. Principles to tailor the saturable and reverse saturable absorption of epsilon-near-zero material[J]. Photonics Research, 2021, 9(5): 678

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    Paper Information

    Category: Optical and Photonic Materials

    Received: Dec. 15, 2020

    Accepted: Feb. 27, 2021

    Published Online: May. 24, 2021

    The Author Email: Yuanan Zhao (yazhao@siom.ac.cn)

    DOI:10.1364/PRJ.417642

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