• Chinese Optics Letters
  • Vol. 19, Issue 3, 031901 (2021)
Yan Guan1, Fang Wang2, Ying Yang2, Deen Wang2, Xin Zhang2, Qiang Yuan2, Dongxia Hu2、3, Xuewei Deng2、3、*, Huaijin Ren4, Yuanlin Zheng1, and Xianfeng Chen1、5、**
Author Affiliations
  • 1State Key Laboratory of Advanced Optical Communication Systems and Networks, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
  • 2Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China
  • 3IFSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China
  • 4Institute of Applied Electronics, China Academy of Engineering Physics, Mianyang 621900, China
  • 5Collaborative Innovation Center of Light Manipulation and Applications, Shangdong Normal University, Jinan 250358, China
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    DOI: 10.3788/COL202119.031901 Cite this Article Set citation alerts
    Yan Guan, Fang Wang, Ying Yang, Deen Wang, Xin Zhang, Qiang Yuan, Dongxia Hu, Xuewei Deng, Huaijin Ren, Yuanlin Zheng, Xianfeng Chen. Variation in linear susceptibility tensor at crystal surface probed by linear Cherenkov radiation[J]. Chinese Optics Letters, 2021, 19(3): 031901 Copy Citation Text show less

    Abstract

    At the surfaces of crystals, linear susceptibility tensors would differ from their counterparts in the interior of the bulk crystal. However, this phenomenon has not been shown in a visible way yet. In previous researches, numerous types of nonlinear Cherenkov radiation based on different materials have been studied, while linear Cherenkov radiation is barely reported. We experimentally prove the generation of linear Cherenkov radiation on the potassium dihydrogen phosphate (KDP) crystal surface and theoretically analyze its phase-matching scheme. In our study, o-polarized light and e-polarized light can mutually convert through the linear Cherenkov process. According to this result, we figure out new nonzero elements at off-diagonal positions in the linear susceptibility tensor matrix at crystal surfaces, compared with the normal form of a bulk KDP.
    P=ε0[χ(1)E+χ(2)E2+χ(3)E3+],

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    nocos[arcsin(sinγno)]=necos[arcsin(sinθ1ne)],

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    necos[arcsin(sinγne)]=nocos[arcsin(sinθ2no)],

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    (PxPyPz)=ε0(χ11000χ11000χ33)(ExEyEz).

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    Pz=ε0[g(z)χ31Ex+g(z)χ32Ey+χ33Ez],

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    g(z)={0,z01,z=0.

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    {u=22(xy),paralleltothelongestedgeofKDPv=22(x+y),opolarizedorientationz=z,

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    Pz=ε0[g(z)22(χ31+χ32)Eu+g(z)22(χ31χ32)Ev+χ33Ez],

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    (u+i2k2z2)A(u,z)=iμ0ε0ω22k[22(χ31χ32)g(z)]Aei(kk)u.

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    S(κz,u)=[u2μ0ε0ω2(χ31χ32)4k]2×A2{sinc[(kkκz22k)u2]}2|G(κz)|2.

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    {u=22(xy),prependiculartothereflectingsurfaceu=22(x+y),paralleltothelongestedgeofKDPz=z,epolarizedorientation;

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    (v+i2k22u)A(v,u)=iμ0ε0ω22k[22(χ31χ32)g(u)]Aei(kk)v,

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    S(κu,v)=[v2μ0ε0ω2(χ31χ32)4k]2×A2{sinc[(kkκu22k)v2]}2·|G(κu)|2.

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    (v+i2k22u)A(v,u)=iμ0ε0ω22k[22(χ13+χ23)g(u)]Aei(kk)v,

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    S(κu,v)=[v2μ0ε0ω2(χ13+χ23)4k]2×A2{sinc[(kkκu22k)v2]}2·|G(κu)|2.

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    Yan Guan, Fang Wang, Ying Yang, Deen Wang, Xin Zhang, Qiang Yuan, Dongxia Hu, Xuewei Deng, Huaijin Ren, Yuanlin Zheng, Xianfeng Chen. Variation in linear susceptibility tensor at crystal surface probed by linear Cherenkov radiation[J]. Chinese Optics Letters, 2021, 19(3): 031901
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