[1]
G.J. Friel R.S. Conney A.J. Kemp, et al. Q-switching of a diode-pumped Nd: YVO4 laser using a quadrupole electro-optic deflector[J]. Appl Phys B, 1998, 67: 267-270.
DOI: 10.1007/s003400050505
Google Scholar
[2]
L. Chen, S. Zhao, H. Zhao. Passively Q-switching of a laser-diode-pumped inrtracavity-frequency-doubling Nd: NYW/KTP laser with GaAs saturable absorber [J]. Opt & Laser Technol, 2003, 35: 563-567.
DOI: 10.1016/s0030-3992(03)00087-2
Google Scholar
[3]
Sipes D L. Highly efficient neodymium: Yttrium aluminum garnet laser end-pumped by a semiconductor laser array[J]. Appl Phys Lett, 1985(47): 74-76.
DOI: 10.1063/1.96256
Google Scholar
[4]
Berger J, Welch D F, Scrifer D R, et al. High power high efficient neodymium: Yttrium aluminum garnet laser end-pumped by a diode array [J]. Appl Phys Lett, 1987(51): 1212-1214.
DOI: 10.1063/1.98733
Google Scholar
[5]
Szabo A,Stein R A. Theory of laser giant pulsing by a saturable absorber[J]. J Appl Phys, 1965(36): 562-1566.
DOI: 10.1063/1.1703087
Google Scholar
[6]
Erickson L E,Szabo A. Effect of saturable absorber lifetime on the performance ofgiant-pulse lasers[J]. J Appl Phys, 1966(37): 4953-4961.
DOI: 10.1063/1.1708172
Google Scholar
[7]
X. Zhang,S. Zhao,Q. Wang, et al. Modeling of passively Q-switched lasers[J]. J Opt Soc AmB, 2000, 17: 1166-1175.
Google Scholar
[8]
Zheng J A,Zhao S Z,Chen L. Influence of thermal effect in gain media on optimumdesign of LD end-pumped solid-solid-state laser[J]. Acta Photonica Siinica., 2001, 30(6): 724-729.
Google Scholar
[9]
J. Zheng,S. Zhao,Q. Wang,X. Zhang, and L. Chen, Laser-diode end-pumped passively O-switcher Nd: YVO4laser withCr4+: YAG saturable absorber, Opt. Eng. 41(9): 2271-2275(2002).
DOI: 10.1117/1.oe.56.8.086111
Google Scholar
[10]
X. Zhang, S. Zhao, Q. Wang, B. Ozygus and H. Weber, Modeling of passively Q-switched lasers, J. Opt. Soc. Am. B, 17(7): 1166-1175 (2000).
DOI: 10.1364/josab.17.001166
Google Scholar