Nonlinear Optical Properties of Perfectly Polarized KIO3 Single Crystal
YIN Xin, LÜ Mengkai, ZHANG Shaojun, LI Fuqi
Institute of Crystal Materials, Shandong University, Jinan 250100
Nonlinear Optical Properties of Perfectly Polarized KIO3 Single Crystal
YIN Xin;LÜ Mengkai;ZHANG Shaojun;LI Fuqi
Institute of Crystal Materials, Shandong University, Jinan 250100
关键词 ：
42.65.Ky
Abstract ： The nonlinear optical properties of a perfectly polarized KIO3 single crystal were investigated. The principal refractive indices and nonlinear optical coeffi-cients have been measured. The results are as follows: n1 =1.6967, n2 =1.8329, n3 =1.8358 for 0.5893μm; d31 =1.2 |d31 (LiIO3 )|, d32 =1.8|d31 (LiIO3 )|. The in-tensity of the frequency-doubled light of the KIO3 single crystal with 2.96rnm thickness is 1.2 times as large as that of the KTP single crystal with the same thickness.
Key words ：
42.65.Ky
出版日期: 1992-02-01
:
42.65.Ky
(Frequency conversion; harmonic generation, including higher-order harmonic generation)
引用本文:
YIN Xin;LÜMengkai;ZHANG Shaojun;LI Fuqi. Nonlinear Optical Properties of Perfectly Polarized KIO3 Single Crystal[J]. 中国物理快报, 1992, 9(2): 77-78.
3 Single Crystal. Chin. Phys. Lett., 1992, 9(2): 77-78.
链接本文:
https://cpl.iphy.ac.cn/CN/
或
https://cpl.iphy.ac.cn/CN/Y1992/V9/I2/77
[1]
CHEN Ji-Gen;LI Chen;CHI Fang-Ping;YANG Yu-Jun;. Single X-Ray Attosecond Pulse Generation by Using Combined Pulses Irradiating on a United Two-Atom System
[2]
GUO Bin;GUO Fu-Quan;CHEN Yong;ZHU Li-Jun;LIU Fu-Sheng;ZHANG Qi-Jin;WANG Gong-Ming. A Simple Model to Describe the Requirement of Realizing All-Optical Poling
[3]
GE Yu-Cheng. Laser Phase Relations of High-Order Harmonic Generation
[4]
JI Feng;;ZHANG Bai-Gang;;LI En-Bang;ZHOU Rui;ZHANG Tie-Li;LU Yang;ZHAO Pu;WANG Peng;YAO Jian-Quan;. A Low-Pump-Threshold High-Repetition-Rate Intracavity Optical Parametric Generator Based on Periodically Poled Lithium Niobate
[5]
WANG Jian;SUN Jun-Qiang;LUO Chuan-Hong;SUN Qi-Zhen;ZHANG Xin-Liang;HUANG De-Xiu. Single-to-Multiple Channel Wavelength Conversions and Tuning of Picosecond Pulses in Quasi-Phase-Matched Waveguides
[6]
ZHANG Xiao-Ming;ZHANG Jing-Tao;BAI Li-Hua;GONG Qi-Huang;XU Zhi-Zhan. A Scaling Law of Photoionization in Ultrashort Pulses
[7]
BO Yong;GENG Ai-Cong;LU Yuan-Fu;YANG Xiao-Dong;PENG Qin-Jun;CUI Qian-Jin;CUI Da-Fu;XU Zu-Yan. A 4.8-W M2 =4.6 Continuous-Wave Intracavity Sum-Frequency Diode-Pumped Solid-State Yellow Laser
[8]
JIN Xiao-Feng;ZHANG Xian-Min. Determination of Zero-Dispersion Wavelength by Four-Wave Mixing
[9]
CHEN Ya-Hui;HOU Wei;PENG Hai-Bo;GENG Ai-Cong;ZHOU Yong;CUI Da-Fu;XU Zu-Yan. Generation of 2.1W Continuous Wave Blue Light by Intracavity Doubling of a Diode-End-Pumped Nd:YAG Laser in a 30mm LBO
[10]
PI Liang-Wen;SHI Ting-Yun;QIAO Hao-Xue. Enhancement of Bichromatic High-Order Harmonic Generation by a Strong Laser Field and Its Third Harmonic
[11]
ZHOU Rui;DING Xin;WEN Wu-Qi;CAI Zhi-Qiang;WANG Peng;YAO Jian-Quan. High-Power Continuous-Wave Diode-End-Pumped Intracavity Frequency Doubled Nd:YVO4 Laser at 671nm with a Compact Three-Element Cavity
[12]
LI Wen-Hui;CHEN Li-Xue;TANG Dong-Hua;DING Wei-Qiang;LIU Shu-Tian. Broadband Frequency Down-Conversion Using Coupled Cavity Structures in One-Dimensional Photonic Crystals
[13]
DENG Xiao-Yuan;WANG Xian-Ju;LIU Han-Ping;ZHUANG Zheng-Fei;GUO Zhou-Yi. Effect of Distribution Pattern of Molecular Dipoles on Microscopic Second-Harmonic Generation
[14]
ZHENG Jun;SHENG Zheng-Ming;ZHANG Jie;CHEN Min;MA Yan-Yun. Effects of Laser Intensities and Target Shapes on Attosecond Pulse Generation from Irradiated Solid Surfaces
[15]
LIU Jun;CHEN Xiao-Wei;ZHU Yi;LENG Yu-Xin;DAI Jun;GE Xiao-Chun;LI Ru-Xin;XU Zhi-Zhan. Compression of Intense Laser Pulse through Filamentation in an Argon-Filled Cell
1992, Vol. 9 
