Calculation of the Spatio-Temporal Dynamics of Q-switched Yb^3+:YAG Laser with an Unstable Cavity and a Super-Gaussian Mirror  

Calculation of the Spatio-Temporal Dynamics of Q-switched Yb^3+:YAG Laser with an Unstable Cavity and a Super-Gaussian Mirror

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作  者:曹丁象 郑万国 王晓峰 於海武 贺少勃 谭吉春 

机构地区:[1]Research Center of Laser Fusion, China Academy of Engineering Physics, PO Box 919-988, Mianyang 621900 [2]College of Optoelectric Science and Engineering, ~Nationa~l University of Defence Technology, Changsha 410073

出  处:《Chinese Physics Letters》2007年第5期1273-1275,共3页中国物理快报(英文版)

基  金:Supported by the National Natural Science Foundation of China under Grant No 10576038.

摘  要:A numerical simulation used to compute the spatio-temporal dynamics of pulse formation of diode-pumped Q- switched Yb: YA G laser is carried out. The model takes the laser amplification and gain saturation, the properties of the laser cavity, and the diffractive effects of the laser disc into account. The numerical calculation is performed for a confocal positive-branch unstable resonator with a super Gaussian coupling mirror. The simulation results show that the laser pulse starts from a Gaussian intensity distribution and becomes rapidly non-Gaussian. The corresponding beam quality M^2 factor is seen to vary approximately from 1.5 at the beginning of the formation of pulse to more than 10 in the tail of the pulse, with a value of 11.6 at the peak of the pulse.A numerical simulation used to compute the spatio-temporal dynamics of pulse formation of diode-pumped Q- switched Yb: YA G laser is carried out. The model takes the laser amplification and gain saturation, the properties of the laser cavity, and the diffractive effects of the laser disc into account. The numerical calculation is performed for a confocal positive-branch unstable resonator with a super Gaussian coupling mirror. The simulation results show that the laser pulse starts from a Gaussian intensity distribution and becomes rapidly non-Gaussian. The corresponding beam quality M^2 factor is seen to vary approximately from 1.5 at the beginning of the formation of pulse to more than 10 in the tail of the pulse, with a value of 11.6 at the peak of the pulse.

分 类 号:TN31[电子电信—物理电子学]

 

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