Journals Articles Conferences News About CLP
Submit a paper Email Alert
Search
Search
Articles
Journals
News
Advanced Search
Top Searches
2D MaterialsTransformation opticsQuantum PhotonicsSmall lasersSemiconductor UV PhotonicsSupersymmetric microring laser arrays

Chinese Optics Letters, Volume. 19, Issue 3, 031901(2021)

Variation in linear susceptibility tensor at crystal surface probed by linear Cherenkov radiation

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
    • show less
    Full TextGet PDF
    Figures&Tables (8)
    Equations (15)
    References (25)
    Cited By (1)
    Tools
    Paper Information
    Topics
    Figures & Tables(8)
    Phase-matching scheme of CSHG.

    Fig. 1. Phase-matching scheme of CSHG.

    Download full size
    View in Article
    (a) Phase-matching scheme of CSHG for oblique incidence. (b) Phase-matching scheme of LCR for oblique incidence.

    Fig. 2. (a) Phase-matching scheme of CSHG for oblique incidence. (b) Phase-matching scheme of LCR for oblique incidence.

    Download full size
    View in Article
    Light path scheme of LCR processes at the KDP surface.

    Fig. 3. Light path scheme of LCR processes at the KDP surface.

    Download full size
    View in Article
    Schematic of the main experiment set-up.

    Fig. 4. Schematic of the main experiment set-up.

    Download full size
    View in Article
    Schematic of KDP placement on the rotation stage.

    Fig. 5. Schematic of KDP placement on the rotation stage.

    Download full size
    View in Article
    Photos of screen (right) and phase-matching analysis (left) of four serial experiments. All of these photos are under the condition that incident beam contains both o- and e- polarization states. (a) Using 1053 nm incident beam; optical axis of KDP is like Fig. 5(a). (b) Using 1053 nm incident beam; optical axis of KDP is like Fig. 5(b). (c) Using 526.5 nm incident beam; optical axis of KDP is like Fig. 5(a). (d) Using 526.5 nm incident beam; optical axis of KDP is like Fig. 5(b).

    Fig. 6. Photos of screen (right) and phase-matching analysis (left) of four serial experiments. All of these photos are under the condition that incident beam contains both o- and e- polarization states. (a) Using 1053 nm incident beam; optical axis of KDP is like Fig. 5(a). (b) Using 1053 nm incident beam; optical axis of KDP is like Fig. 5(b). (c) Using 526.5 nm incident beam; optical axis of KDP is like Fig. 5(a). (d) Using 526.5 nm incident beam; optical axis of KDP is like Fig. 5(b).

    Download full size
    View in Article
    Theoretical predictions and measured results in the experiment on the relationship of external LCR emitting angles θ1 and θ2.

    Fig. 7. Theoretical predictions and measured results in the experiment on the relationship of external LCR emitting angles θ1 and θ2.

    Download full size
    View in Article

    • Table 1. The Relationship of Polarization State and Nonzero Elements

      View table
      View in Article

      Table 1. The Relationship of Polarization State and Nonzero Elements

      Optical Axis OrientationConversion TypeIncident Electric Field ComponentsLCR Electric Field ComponentsNew Nonzero Elements in χ(1) (underlined)Remarks
      Figure 5(a)o to eEx & EyEx, Ey, & Ez(χ11000χ110χ31χ32χ33)χ31, χ32 cannot be zero at the same time
      e to oEx, Ey, & EzEx & Ey(χ11000χ11000χ33)No new nonzero element is necessary simply considering the polarization state
      Figure 5(b)o to eEx & EyEz(χ11000χ110χ31χ32χ33)χ31, χ32 cannot be zero at the same time
      e to oEzEx or Ey or Ex & Ey(χ110χ130χ11χ2300χ33)χ13, χ23 cannot be zero at the same time
    Tools

    Get Citation

    Copy Citation Text

    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," Chin. Opt. Lett. 19, 031901 (2021)

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Set citation alerts for article
    Save article for my favorites
    Paper Information

    Category: Nonlinear Optics

    Received: Aug. 5, 2020

    Accepted: Jan. 27, 2021

    Published Online: Mar. 11, 2021

    The Author Email: Xuewei Deng (xwdeng@caep.com), Xianfeng Chen (xfchen@sjtu.edu.com)

    DOI:10.3788/COL202119.031901

    Topics

    laser devices and laser physics
    Lasers and Laser Optics
    Laser physics
    laser manufacturing
    Instrumentation, Measurement and Metrology