LD-end-pumped passively Q-switched Nd:YAG ceramic laser with single wall carbon nanotube saturable absorber

Abstract We report on a LD-end-pumped passively Q-switched Nd:YAG ceramic laser by using a novel single wall carbon nanotube saturable absorber (SWCNT-SA). The SWCNT wafer was fabricated by electric Arc discharge method on quartz substrate with absorption wavelength of 1064 nm. We firstly investigated the continuous wave (CW) laser performance and scattering properties of Nd:YAG ceramic sample. For the case of passively Q-switched operation, a maximum output power of 376 mW was obtained at an incident pump power of 8.68 W at 808 nm, corresponding to an optical–optical conversion efficiency of 4.3%. The repetition rate as the increase of pump power varied from 14 to 95 kHz. The minimum pulse duration of 1.2 μs and maximum pulse energy of 4.5 μJ was generated at a repetition rate of 31.8 kHz.

[1]  M. Lavan High Energy Laser Systems for Short Range Defense , 2009 .

[2]  K. Liu,et al.  LD end-pumped passively mode-locked Nd:YVO4 laser with single-walled carbon nanotubes , 2011 .

[3]  Jun Wang,et al.  Carbon nanotubes and nanotube composites for nonlinear optical devices , 2009 .

[4]  Yubai Pan,et al.  Scattering effect and laser performance for the Nd:YAG transparent ceramics , 2011 .

[5]  Horst Weber,et al.  Investigation of a passive Q‐switched, externally controlled, quasicontinuous or continuous pumped Nd:YAG laser , 1996 .

[6]  Akio Ikesue,et al.  Fabrication and Optical Properties of High‐Performance Polycrystalline Nd:YAG Ceramics for Solid‐State Lasers , 1995 .

[7]  Zhang Xiao-Fu,et al.  Comparison of Nd:YAG Ceramic Laser Pumped at 885 nm and 808 nm , 2009 .

[8]  Dafu Cui,et al.  A kilowatt level diode-side-pumped QCW Nd:YAG ceramic laser , 2010 .

[9]  H. Zhang,et al.  Diode-pumped passively Q-switched Nd:YVO4 laser with a carbon nanotube saturable absorber , 2011 .

[10]  Yonggang Wang,et al.  Diode-pumped passively Q-switched Nd:Lu0.33Y0.37Gd0.3VO4 laser using a single-walled carbon nanotube saturable absorber , 2011 .

[11]  Ken-ichi Ueda,et al.  Neodymium doped yttrium aluminum garnet (Y3Al5O12) nanocrystalline ceramics—a new generation of solid state laser and optical materials , 2002 .

[12]  Jie Liu,et al.  High power ultrafast Nd:YVO4 laser mode locked by single wall carbon nanotube absorber , 2011 .

[13]  Bo Dong,et al.  Tunable Passively $Q$-switched Erbium-Doped Fiber Laser With Carbon Nanotubes as a Saturable Absorber , 2010, IEEE Photonics Technology Letters.

[14]  Yonggang Wang,et al.  2 μm passive Q-switched mode-locked Tm3+:YAP laser with single-walled carbon nanotube absorber , 2012 .

[15]  V. Lupei Ceramic laser materials and the prospect for high power lasers , 2009 .

[16]  Y. Liu,et al.  Passively Q-Switched Yb:YAG Laser with Cr(4+):YAG as the Saturable Absorber. , 2001, Applied optics.

[17]  Zhipei Sun,et al.  A stable, wideband tunable, near transform-limited, graphene-mode-locked, ultrafast laser , 2010 .

[18]  David J. Richardson,et al.  Passively Q-switched 0.1mJ fiber laser system at 1.53µm , 1999 .

[19]  F. Kärtner,et al.  56-ps passively Q-switched diode-pumped microchip laser. , 1997, Optics letters.

[20]  Shengzhi Zhao,et al.  Optimization of dye Q-switched lasers , 1994 .

[21]  A. Ferrari,et al.  Graphene Photonics and Optoelectroncs , 2010, CLEO 2012.