摘要
A diode end-pumped acousto-optic Q-switched Nd:YVO_4/LuVO_4 Raman laser is demonstrated. Both YVO_4 and LuVO_4 can work as Raman gain, and slightly different active vibration modes of both crystals can result in different first-Stokes wavelengths. The output characteristic as the Raman competition between YVO_4 and LuVO_4 crystals for the laser systems with both shared cavity and coupled cavity is experimentally investigated.For the shared cavity, simultaneous Raman conversion in both YVO_4 and LuVO_4 crystals is achieved with dualwavelength emission at 1175.8 and 1177.1 nm. The maximum output power of 1.03 W and the conversion efficiency of 10.3% are obtained. The 0.84 W single first Stokes wavelength at 1177.1 nm with LuVO_4 Raman conversion is achieved with the coupled cavity. The results show that the coupled cavity with short Raman cavity can obtain a narrow pulse width. The separated laser crystal and Raman gain media with different vanadates in shared cavity have advantages in achieving dual-wavelength lasers with small frequency intervals.
A diode end-pumped acousto-optic Q-switched Nd:YVO_4/LuVO_4 Raman laser is demonstrated. Both YVO_4 and LuVO_4 can work as Raman gain, and slightly different active vibration modes of both crystals can result in different first-Stokes wavelengths. The output characteristic as the Raman competition between YVO_4 and LuVO_4 crystals for the laser systems with both shared cavity and coupled cavity is experimentally investigated.For the shared cavity, simultaneous Raman conversion in both YVO_4 and LuVO_4 crystals is achieved with dualwavelength emission at 1175.8 and 1177.1 nm. The maximum output power of 1.03 W and the conversion efficiency of 10.3% are obtained. The 0.84 W single first Stokes wavelength at 1177.1 nm with LuVO_4 Raman conversion is achieved with the coupled cavity. The results show that the coupled cavity with short Raman cavity can obtain a narrow pulse width. The separated laser crystal and Raman gain media with different vanadates in shared cavity have advantages in achieving dual-wavelength lasers with small frequency intervals.
引文
[1] Piper J A and Pask H M 2007 IEEE J. Sel. Top. Quantum Electron. 13 692
[2] Hisamuddin N, Zakaria U N, Zulkifli M Z, Latif A A, Ahmad H and Harun S W 2016 Chin. Phys. Lett. 33 074208
[3] Li F, Zhao W Q, Qiao X, Xia C Q, Wang L C, Fan H B and Shen M Y 2016 Chin. Phys. B 25 114207
[4] Su F F, Zhang X Y, Wang Q P, Chang J, Jia P, Li S T,Zhang X L and Cong Z H 2007 Chin. Phys. B 16 3370
[5] Men S J, Liu Z J, Cong Z H, Liu Y, Xia J B, Zhang S S,Cheng W Y, Li Y F, Tu C Y and Zhang X Y 1988 Opt.Lett. 13 530
[6] Duan Y M, Zhu H Y, Zhang Y J, Zhang G, Zhang J, Tang D Y and Kaminskii A A 2016 Sci. Rep. 6 33852
[7] Frank M, Smetanin S N, Jelínek M, Vyhlídal D, Ivleva L I,Zverev P G and Kube?ek V 2018 Opt. Lett. 43 2527
[8] Liu Y, Liu Z J, Cong Z H, Men S J, Xia J B, Rao H and Zhang S S 2015 Chin. Phys. Lett. 32 124201
[9] Kaminskii A A, Ueda K, Eichler H J, Kuwano Y, Kouta H,Bagaev S N, Chyba T H, Barnes J C, Gad G M A, Murai T and Lu J 2001 Opt. Commun. 194 201
[10] Chen Y F 2004 Opt. Lett. 29 1915
[11] Zhu H Y, Guo J H, Ruan X K, Xu C W, Duan Y M, Zhang Y J and Tang D Y 2017 IEEE Photon. J. 9 1500807
[12] Lee C Y, Chang C C, Cho C Y, Tuan P H and Chen Y F2015 IEEE J. Sel. Top. Quantum Electron. 21 1600305
[13] Lee A J, Lin J and Pask H M 2010 Opt. Lett. 35 3000
[14] Zhu H Y, Guo J H, Duan Y M, Zhang J, Zhang Y C, Xu C W, Wang H Y and Fan D Y 2018 Opt. Lett. 43 345
[15] Zhang X, Zhang Y C, Li J, Li R J, Song Q K, Zhang J L and Fan L 2017 Acta Phys. Sin. 66 194203(in Chinese)
[16] Zhang Y J et al 2011 Acta Phys. Sin. 60 094209(in Chinese)
[17] Kaminskii A A, Rhee H, Eichler H J, Ueda K, Oka K and Shibata H 2008 Appl. Phys. B 93 865
[18] Kaminskii A A, Bettinelli M, Dong J, Jaque D and Ueda K2009 Laser Phys. Lett. 6 374
[19] Rao R, Garg A B, Sakuntala T, Achary S N and Tyagi A K 2009 J. Solid State Chem. 182 1879
[20] Xu M, Yu H H, Zhang H J, Xu X G and Wang J Y 2011 J.Rare Earths 29 207
[21] Kaminskii A A, Lux O, Rhee H, Eichler H J, Ueda K,Yoneda H, Shirakawa A, Zhao B, Chen J, Dong J and Zhang J 2012 Laser Phys. Lett. 9 879
[22] Dimitrov D Z, Rafailov P M, Chen Y F, Lee C S, Todorov R and Juang J Y 2017 J. Cryst. Growth 473 34
[23] LüY F, Zhang X H, Li S T, Xia J, Cheng W B and Xiong Z 2010 Opt. Lett. 35 2964
[24] Tan Y, Fu X H, Zhai P and Zhang X H 2013 Laser Phys.23 045806
[25] Jiang W, Zhu S Q, Chen X Z, Liu Y M, Che Z Q, Yin H,Li Z, Wang S and Chen Y H 2014 Appl. Opt. 53 1328
[26] Duan Y M, Zhu H Y, Wang H Y, Zhang Y J and Chen Z Q 2016 Opt. Express 24 5565
[27] Cai W Y, Duan Y M, Li J T, Yan L F, Mao M J, Zhao B and Zhu H Y 2015 Chin. Phys. Lett. 32 034206
[28] Zhang Y C, Fan L, Wei C F, Min X and Ren S X 2018 Acta Phys. Sin. 67 024206(in Chinese)
[29] Zhang H N, Chen X H, Wang Q P and Li P 2015 Chin.Phys. Lett. 32 014203
[30] Su K W, Chang Y T and Chen Y F 2007 Appl. Phys. B 8847
[31] Zhang Y Y, Huo Y J, He S F and Gong K 2010 Chin. Phys.Lett. 27 124207
[32] Chen J B, Zhu H B, Xia W, Guo D M, Hao H and Wang M 2017 Opt. Express 25 560
[33] Zhao P, Ragam S, Ding Y J and Zotova I B 2011 Opt. Lett.36 4818