• Photonics Research
  • Vol. 9, Issue 10, 2060 (2021)
Zhengji Wen1, Jialiang Lu1, Weiwei Yu1, Hao Wu2, Hao Xie1, Xiaohang Pan1, Qianqian Xu1, Ziji Zhou1, Chong Tan1, Dongjie Zhou1, Chang Liu2, Yan Sun1、5, Ning Dai1、3, and Jiaming Hao1、4、*
Author Affiliations
  • 1State Key Laboratory of Infrared Physics, Shanghai Institute of Technical Physics, Chinese Academy of Sciences, Shanghai 200083, China
  • 2Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education, School of Physics and Technology, Wuhan University, Wuhan 430072, China
  • 3Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou 310024, China
  • 4Institute of Precision Optical Engineering, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
  • 5e-mail: sunny@mail.sitp.ac.cn
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    DOI: 10.1364/PRJ.438095 Cite this Article Set citation alerts
    Zhengji Wen, Jialiang Lu, Weiwei Yu, Hao Wu, Hao Xie, Xiaohang Pan, Qianqian Xu, Ziji Zhou, Chong Tan, Dongjie Zhou, Chang Liu, Yan Sun, Ning Dai, Jiaming Hao. Dynamically reconfigurable subwavelength optical device for hydrogen sulfide gas sensing[J]. Photonics Research, 2021, 9(10): 2060 Copy Citation Text show less

    Abstract

    The importance of tunable subwavelength optical devices in modern electromagnetic and photonic systems is indisputable. Herein, a lithography-free, wide-angle, and reconfigurable subwavelength optical device with high tunability operating in the near-infrared regions is proposed and experimentally demonstrated, based on a reversible nanochemistry approach. The reconfigurable subwavelength optical device basically comprises an ultrathin copper oxide (CuO) thin film on an optical thick gold substrate by utilizing the reversible chemical conversion of CuO to sulfides upon exposure to hydrogen sulfide gas. Proof-of-concept experimental results show that the maximal modulation depth of reflectance can be as high as 90% at the wavelength of 1.79 μm with the initial thickness of CuO taken as 150 nm. Partially reflected wave calculations combined with the transfer matrix method are employed to analytically investigate the optical properties of the structure, which show good agreement with experimental results. We believe that the proposed versatile approaches can be implemented for dynamic control management, allowing applications in tunable photonics, active displays, optical encryption, and gas sensing.
    CuO+H2SCuS+H2O,

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    CuO+H2S0.5Cu2S+H2O+0.5S.

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    CuS+1.5O2CuO+SO2.

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    r=r˜01+r˜12e2iβ˜1+r˜23e2iβ˜2(r˜01r˜12+e2iβ˜1)1+r˜01r˜12e2iβ˜1+r˜23e2iβ˜2(r˜12+r˜01e2iβ˜1),

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    r=r0+r1+r2+r3+=n=0rn.

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    ΔRrel=|RiRiii|Ri×100%,

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    r=r˜0123=r˜01+r˜123e2iβ˜11+r˜01r˜123e2iβ˜1,(B1)

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    r˜123=r˜12+r˜23e2iβ˜21+r˜12r˜23e2iβ˜2.(B2)

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    r˜jk={NjcosθjNkcosθkNjcosθj+Nkcosθkfor  TE  polarizationNkcosθjNjcosθkNkcosθj+Njcosθkfor  TM  polarization(B3)

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    β˜1=2πλN1h1cosθ1,β˜2=2πλN2h2cosθ2.(B4)

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    r=r0+r1+r2+r3+=n=0rn,(B5)

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    rn={r˜01for  n=0t˜01t˜10r˜123nr˜10n1e2inβ˜1for  n1.(B6)

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    t˜jk={2NjcosθjNjcosθj+Nkcosθkfor  TE  polarization2NjcosθjNkcosθj+Njcosθkfor  TM  polarization.(B7)

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    R=|r0+r1+r2+r3+|2=|r|2.(B8)

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    Zhengji Wen, Jialiang Lu, Weiwei Yu, Hao Wu, Hao Xie, Xiaohang Pan, Qianqian Xu, Ziji Zhou, Chong Tan, Dongjie Zhou, Chang Liu, Yan Sun, Ning Dai, Jiaming Hao. Dynamically reconfigurable subwavelength optical device for hydrogen sulfide gas sensing[J]. Photonics Research, 2021, 9(10): 2060
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