期刊文献+

碳基吸收体被动锁模大功率皮秒激光器 被引量:6

High Power Picosecond Lasers Mode Locked with Carbon Based Absorbers
原文传递
导出
摘要 采用垂直蒸发法分别在玻璃和石英衬底上淀积单壁碳纳米管和氧化石墨烯材料来制作碳基可饱和吸收体。利用单壁碳纳米管作为饱和吸收体,实现了Nd:YVO4激光器被动锁模,最高输出功率为3.6 W,斜率效率为31%,脉冲宽度为7.6ps,重复频率为75MHz。利用氧化石墨烯作为可饱和吸收体,实现了Nd:GdVO4激光器被动锁模,最大输出功率为1.1W,斜率效率为11.3%,脉冲宽度为4.5ps,重复频率为70MHz。 Single walled carbon nanotubes and graphene oxide are deposited on glass and quartz by vertical evaporation method, respectively. By using single walled carbon nanotubes absorber, passively mode locked Nd YVO4 laser is obtained. The maximum output power is 3.6 W, the slope efficiency is 31%, the pulse duration is 7.6 ps and the repetition rate is 75 MHz. By using graphene oxide absorber, passively mode locked Nd: GdV04 laser is achieved. The maximum output power is 1.1 W, the slope efficiency is 11.3 %, the pulse duration is 4.5 ps and the repetition rate is 70 MHz.
出处 《中国激光》 EI CAS CSCD 北大核心 2012年第7期1-4,共4页 Chinese Journal of Lasers
基金 国家自然科学基金(61078032) 香港理工大学基金(G-YJ20)资助课题
关键词 激光器 碳纳米管 氧化石墨烯 锁模 大功率 固体激光器 lasers carbon nanotubes graphene oxide mode locking high power solid-state laser
  • 相关文献

参考文献11

  • 1U. Keller, D. A. B. Miller, G. D. Boyd et al.. Solid-state low-loss intracavity saturable absorber for NdYLF lasers: an A-FPSA[J].Opt. Lett., 1992, 17(7): 505-507.
  • 2陈檬,张丙元,李港,王勇刚.半导体可饱和吸收镜被动锁模Nd∶YAG激光器的研究[J].中国激光,2004,31(6):646-648. 被引量:21
  • 3李霄,王勇刚,张世强,汪晓波,许晓军.半导体可饱和吸收镜被动锁模侧面抽运Nd∶YAG激光器研究[J].光学学报,2009,29(11):3103-3107. 被引量:9
  • 4S. Iijima. Helical microtubeles of graphitic carbon[J].Nature, 1991, 354(6348): 56-58.
  • 5Y. Sakakibara, Aleksey, G. Rozhin et al.. Carbon nanotube-poly(vinylalcohol) nanocomposite film devices: applications for femtosecond fiber laser mode lockers and optical amplifier noise suppressors[J].Jpn. J. Appl. Phys., 2005, 44(4A): 1621-1625.
  • 6H. Zhang, D. Y. Tang, L. M. Zhao et al.. Large energy mode locking of an erbium-doped fiber laser with atomic layer graphene[J].Opt. Express, 2009, 17(20): 17630-17635.
  • 7Q. L. Bao, H. Zhang, J. X. Yang et al.. Graphene-polymer nanofiber membrane for ultrafast photonics[J].Adv. Funct. Mater., 2010, 20(5): 782-791.
  • 8W. D. Tan, C. Y. Su, R. J. Knize et al.. Mode locking of ceramic Ndyttrium aluminum garnet with graphene as a saturable absorber[J].Appl. Phys. Lett., 2010, 96(3): 031106.
  • 9J. L. Xu, X. L. Li, Y. Z. Wu et al.. Graphene saturable absorber mirror for ultra-fast-pulse solid-state laser[J].Opt. Lett., 2011, 36(20): 1948-1950.
  • 10C. C. Liu, Y. G. Wang, J. Liu et al.. Ultrafast YbY2SiO5 laser investigation based on a carbon nanotube absorber[J].Appl. Opt., 2011, 50(19): 3229-3232.

二级参考文献33

  • 1陈檬,张丙元,李港,王勇刚.半导体可饱和吸收镜被动锁模Nd∶YAG激光器的研究[J].中国激光,2004,31(6):646-648. 被引量:21
  • 2张丙元,陈檬,李港,郭晓萍,于海娟,宋海平,王勇刚.激光二极管侧面抽运Nd∶YAG锁模激光器的研究[J].光学学报,2005,25(1):59-62. 被引量:20
  • 3陆燕玲,杨扬,王俊,董安平,李胜华,孙宝德,周然,戴顺波.Tm∶YAP激光晶体光谱参数的计算[J].中国激光,2006,33(7):968-972. 被引量:7
  • 4N. P. Barnes, W. J. Rodriguez, B. M. Walsh. Ho:Tm:YLF laseramplifiers[J]. J. Opt. Soc. Am. B, 1996, 13(12): 2872-2882.
  • 5B. M. Walsh, N. P. Barnes, B. D. Bartolo. The temperature dependence of energy transfer between the Tm a F4 and Ho 517 manifolds of Tin-sensitized Ho luminescence in YAG and YLF 2000, 90(1-2) : 39-48.
  • 6R. Gunnar, S. Knut. Modeling of laser-pumped Tm and Ho lasers accounting for upconversion and ground state depletion[J]. IEEE J. Quantum Electron., 1996, 32(9): 1645-1656.
  • 7J. G. Wang, Z. G. Zhang, J. Z. Xu et al.. Spectroscopic investigation on the properties of visible and near infrared emissions in Tm^3+ , Ho^3+ co doped YVO4 crystals[J]. Chinese Phys. , 2000, 9(3): 210-215.
  • 8C. Nagasawa, D. Sakaizawa, H. Hara et al.. Lasing characteristics of a CW Tin, Ha : YLF double cavity microchip laser[J]. Opt. Commun. , 2004, 234:301-304.
  • 9J. Izawa, H. Nakajima, H. Hara et al.. Comparison of lasing performance of Tm, Ho: YLF laser by use of single and double cavities[J]. Appl. Opt., 2000, 39(15): 1418-1421.
  • 10E. Kato, H. Noguchi, M. Nagai et al.. Significant progress in II VI blue green laser diode lifetime[J]. Electron. Lett. , 1998, 34(3) : 282-284.

共引文献34

同被引文献63

  • 1陈檬,张丙元,李港,王勇刚.半导体可饱和吸收镜被动锁模Nd∶YAG激光器的研究[J].中国激光,2004,31(6):646-648. 被引量:21
  • 2严钢,刘之景,王克逸,刘磁辉.半导体单壁碳纳米管光电特性研究新进展[J].激光技术,2005,29(2):196-198. 被引量:1
  • 3曹轶乐,于丽,杨伯君.固体激光器中色散与自相位调制对脉冲的影响[J].激光技术,2005,29(3):248-250. 被引量:3
  • 4王旌,张洪明,张鋆,燕萌,姚敏玉.基于饱和吸收镜的被动锁模光纤激光器[J].中国激光,2007,34(2):163-165. 被引量:32
  • 5U. Keller, W. H. Knox, H. Roskos. Coupled-cavity resonant passive mode-locked Ti r sapphire laser] I}, Opt. Lett. ,1990, 15 (23): 1377 - 1379.
  • 6N. Metzger, C. Leburn, A. Lagatskyet al . Femtosecond pulse generation around 1500 nm using a GaInNAsSb SESAM [J]. Opt. Express, 2008, 16(23): 18739- 18744.
  • 7C. J. Saraceno, O. H. Heck!, C. R. E. Baer et al . SESAMs for high-power femtosecond modelocking , power scaling of an Yb : LUSC03 thin disk laser to 23 Wand 235 fs] L]. Opt. Express, 2011, 19(21): 20288-20300.
  • 8F. -Q. Li , K. Liu , L. Han et al . High-power 880-nm diode-directly-pumped passively mode-locked Nd s YVO, laser at 1342 nm with a semiconductor saturable absorber mirror [J]' Opt. Lett. ,2011,36(8): 1485-1487.
  • 9F. Fusari , A. Lagatsky , G. Jose et al . Femtosecond mode-locked TmH and TmH - HoH doped 2 Ilm glass lasers] ]"]. Opt. Express, 2010,18(21): 22090-22098.
  • 10H. Haus. Theory of mode locking with a slow saturable absorber [J]. IEEE J. Quantum Electron., 1975, 11(9): 736-746.

引证文献6

二级引证文献17

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部