摘要
We report a high conversion efficiency Q-switched Nd:YVO_4/KTiOAsO_4(KTA) intracavity optical parametric oscillator(IOPO) operating near 3.5 um based on direct 880 nm laser diode(LD) pumping. A maximum average idler output power of 2.6 W with a pulse width of about 7.9 ns is achieved under an absorbed LD power of 45.4 W at a pulse repetition rate(PRR) of 10 kHz. The maximum optical-optical conversion efficiency from LD power to OPO mid-infrared(MIR) output of 6.74% is achieved. To our knowledge, this is the highest conversion efficiency for a KTA-IOPO by exploiting a Q-switched laser as the parent fundamental pump source. The beam quality factors M~2 of the MIR beam at the full output power with a PRR of 10 kHz are within 2.12 in both the horizontal and vertical directions, indicating a near Gaussian mode.
We report a high conversion efficiency Q-switched Nd:YVO_4/KTiOAsO_4(KTA) intracavity optical parametric oscillator(IOPO) operating near 3.5 um based on direct 880 nm laser diode(LD) pumping. A maximum average idler output power of 2.6 W with a pulse width of about 7.9 ns is achieved under an absorbed LD power of 45.4 W at a pulse repetition rate(PRR) of 10 kHz. The maximum optical-optical conversion efficiency from LD power to OPO mid-infrared(MIR) output of 6.74% is achieved. To our knowledge, this is the highest conversion efficiency for a KTA-IOPO by exploiting a Q-switched laser as the parent fundamental pump source. The beam quality factors M~2 of the MIR beam at the full output power with a PRR of 10 kHz are within 2.12 in both the horizontal and vertical directions, indicating a near Gaussian mode.
引文
[1]Liu J,Liu Q,Yan X,Chen H and Gong H 2010 Laser Phys.Lett.7 630
[2]Chen D W and Masters K 2001 Opt.Lett.26 25
[3]Lancaster D G 2009 Opt.Commun.282 272
[4]Zhang B G,Xu D G,Wang P,Feng J,Zhang T L and Yao J Q 2008 Chin.Phys.B 17 633
[5]Yao B Q,Shen Y J,Duan X M,Dai T Y,Ju Y L and Wang Y Z 2014 Opt.Lett.39 6589
[6]Xiong B,Guo L,Hou W,Lin X C and Li J M 2011 Laser Phys.21 362
[7]Duan Y M,Zhu H Y,Ye Y L,Zhang D,Zhang G and Tang D Y 2014 Opt.Lett.39 1314
[8]Miao J G,Peng J Y,Wang B S and Tan H M 2008 Appl.Opt.47 4287
[9]Dong X L,Zhang B T,He J L,Huang H T,Yang K J,Xu J L,Zuo C H,Zhao S,Qiu G and Liu Z L 2009 Opt.Commun.282 1668
[10]Wu R F,Lai K S,Wong H F,Xie W J,Lim Y L and Lau E 2001 Opt.Express 8 694
[11]Bai F,Wang Q P,Liu Z J,Zhang X Y,Lan W X,Tao X Tand Sun Y X 2013 Appl.Phys.B 112 83
[12]Zhong K,Yao J Q,Xu D G,Wang J L,Li J S and Wang P 2010 Appl.Phys.B 100 749
[13]Frede M,Wilhelm R and Kracht D 2006 Opt.Lett.31 3618
[14]Cui L,Zhang H L,Xu L,Li J,Yan Y,Duan C,Sha P Fand Xin J G 2010 Chin.Phys.Lett.27 114204
[15]Mao Y F,Zhang H L,Xu L,Deng B,Xing J C,Xin J Gand Jiang Y 2014 Chin.Phys.Lett.31 074206
[16]Sheng Q,Ding X,Shi C P,Yin S J,Li B,Shang G,Yu XY,Wen W Q and Yao J Q 2012 Opt.Express 20 8041
[17]Peng X Y,Xu L and Asundi A 2005 IEEE J.Quantum Electron.41 53
[18]Bai F,Wang Q P,Liu Z J,Zhang X Y,Wan X B,Lan WX,Jin G F,Tao X T and Sun Y X 2012 Opt.Express 20807