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DENG Cheng-xian, LI Zheng-jia, ZHU Chang-hong. Passively Q-switched intracavity single resonant optical parametric oscillator and Cr4+:YAG laser[J]. LASER TECHNOLOGY, 2005, 29(6): 589-593.
Citation: DENG Cheng-xian, LI Zheng-jia, ZHU Chang-hong. Passively Q-switched intracavity single resonant optical parametric oscillator and Cr4+:YAG laser[J]. LASER TECHNOLOGY, 2005, 29(6): 589-593.

Passively Q-switched intracavity single resonant optical parametric oscillator and Cr4+:YAG laser

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  • Received Date: September 20, 2004
  • Revised Date: January 12, 2005
  • Published Date: November 24, 2005
  • The characteristics of the Cr4+:YAG laser and single resonant optical parametric oscillator(SRO) pumped intracavity by a passively Q-switched Nd3+:YAG laser are analyzed using Cr4+:YAG as the saturable absorber and laser gain medium.The rate equations describing the dynamic characteristics of this kind of laser and intracavity SRO(ICSRO) are set up.Under suitable conditions,the Cr4+:YAG laser gain medium can amplify the SRO signal wave generated in the second-order nonlinear interacting process if the wavelength of this wave is in the range of the gain spectra of Cr4+:YAG.The influence of intermediate level on the Cr4+:YAG saturable absorber and laser as well as ICSRO are considered in the analysis.This intermediate level between the higher excited state and the upper laser level has a relaxing time constant of approximate 100ns.
  • [1]
    YASHKIR Y,DRIEL H M V.Passively Q-switched 1.57μm intracavity optical parametric oscillator[J].Appl Opt,1999,38(12):2554~2559.
    [2]
    EILERS H,DENNIS W M,YEN W M et al.Performance of a Cr:YAG laser[J].IEEE J Q E,1993,29(9):2508~2512.
    [3]
    SPARIOSU K,CHEN W,STULTZ R et al.Dual Q-switching and laser action at 1.06 and 1.44 μm in a Nd3+YAG-Cr4+:YAG oscillator at 300K[J].Opt Lett,1993,18(10):814~816.
    [4]
    SUDA A,KADOI A,NAGASAKA K et al.Absorption and oscillation characteristics of a pulsed Cr4+:YAG laser investigated by a double-pulse pumping technique[J].IEEE J Q E,1999,35(10):1548~1553.
    [5]
    王加贤,吕凤萍,苏娅菲.双调Q复合腔Nd:YAG-Gr4+:YAG激光器的研究[J].中国激光,2004,31(4):399~402.
    [6]
    DEBUISSCHERT T,RAFFY J,POCHOLLE J P et al.Intracavity optical parametric oscillator:study of the dynamics in pulsed regime[J].J O S A.1996,B13(7):1569~1587.
    [7]
    CHEN Y F,LAN Y P,CHANG H L.Analytical model for design criteria of passively Q-switched lasers[J].IEEE J Q E,2001,37(3):462~468.
    [8]
    PATEL F D,BEACH R J.New formalism for the analysis of passively Q-switched laser systems[J].IEEE J Q E,2001,37(5):707~715.
    [9]
    ZOTOVA I B,DING Y J,MU X D et al.Reductions of threshold for a mid-infrared optical parametric oscillator by an intracavity optical amplifier[J].Opt Lett,2003,28(7):552~554.
    [10]
    SMITH A V,ARMSTRONG D J,ALFORD W J.Increased acceptance bandwidths in optical frequency conversion by use of multiple walk-off-compensating nonlinear crystals[J].J O S A,1998,B15(1):122~141.
    [11]
    程勇,陈波.加固型人眼安全OPO激光器的设计[J].激光技术,2004,28(1):91~93.
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