LI De-Hua1, WANG Ling1, GAO Chun-Qing1,5, ZHANG Zhi-Guo1, FENG Bao-Hua1, Volker Gaebler2, LIU Bai-Ning2, H. J. Eichler2, ZHANG Shi-Wen3, LIU An-Han3, SHEN De-Zhong4
1Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080
2Optical Institute, Technical University Berlin, Strasse de 17 Juni 135, D-10623 Berlin, Germany
3North China Research Institute of Electro-Optics, Beijing 100015
4Research Institute of Synthetic Crystal, P.O. Box 733, Beijing 100018
5Optical Engineering Department, Beijing Institute of Technology, Beijing 100081 Permanent address
LI De-Hua1;WANG Ling1;GAO Chun-Qing1,5;ZHANG Zhi-Guo1;FENG Bao-Hua1;Volker Gaebler2;LIU Bai-Ning2;H. J. Eichler2;ZHANG Shi-Wen3;LIU An-Han3;SHEN De-Zhong4
1Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080
2Optical Institute, Technical University Berlin, Strasse de 17 Juni 135, D-10623 Berlin, Germany
3North China Research Institute of Electro-Optics, Beijing 100015
4Research Institute of Synthetic Crystal, P.O. Box 733, Beijing 100018
5Optical Engineering Department, Beijing Institute of Technology, Beijing 100081 Permanent address
Abstract: We carried out the operation of an intracavity frequency-doubled self-Q-switched Nd,Cr:YAG/KNbO3 946/473nm microchip laser pumped by a Ti:sapphire laser. The overall cavity length was about 4 mm. The maximum average blue power of 12 mW was achieved with a repetition rate of 13 kHz at an absorbed pump power of 545 mW. The pulses of 473 nm laser had duration of 7ns and peak power of 132 W at this pump level. The conversion efficiency was 2.2 % with respect to absorbed pump power of 808 nm laser.