7.6  W 1342  nm passively mode-locked picosecond composite Nd:YVO4/YVO4 laser with a semiconductor saturable absorber mirror.

A high average power 1342 nm passively CW mode-locked picoseconds (ps) composite Nd:YVO4 laser was demonstrated with a semiconductor saturable absorber mirror (SESAM). The oscillator cavity was carefully designed to optimize the laser beam radii in the crystal and on the SESAM. The combination of composite bonded laser crystal, direct pumping, and dual end-pumped configuration was adopted to reduce the thermal effect and produce high output power with high beam quality. A maximum average output power of 7.63 W was obtained with a repetition rate of 77 MHz and a pulse duration of 24.2 ps under an absorbed pump power of 38.6 W, corresponding to an optical-optical efficiency of 19.7% and a slope efficiency of 25.9%, respectively. The beam quality factor M(2) was measured to be 1.49.

[1]  K. Weingarten,et al.  Diode-pumped passively mode-locked 1.3-microm Nd:YVO(4) and Nd:YLF lasers by use of semiconductor saturable absorbers. , 1996, Optics letters.

[2]  O. Musset,et al.  Flashlamp-pumped Nd:KGW laser at repetition rates up to 50 Hz , 1997 .

[3]  Alphan Sennaroglu Efficient continuous-wave operation of a diode-pumped Nd:YVO4 laser at 1342 nm , 1999 .

[4]  Y. Lan,et al.  Efficient high-power diode-end-pumped TEM/sub 00/ Nd:YVO4 laser , 1999, IEEE Photonics Technology Letters.

[5]  Yung-Hsin Chen,et al.  Study of high-power diode-end-pumped Nd:YVO4 laser at 1.34 μm: influence of Auger upconversion , 1999 .

[6]  A. Di Lieto,et al.  A 7-W diode-pumped Nd:YVO4 cw laser at 1.34 μm , 2002 .

[7]  Dafu Cui,et al.  Double-end-pumped 11-W Nd:YVO4 cw laser at 1342 nm , 2005 .

[8]  Minhua Jiang,et al.  Continuous-wave laser performance of Nd:LuVO 4 crystal operating at 1.34 µm , 2005 .

[9]  J. L. He,et al.  Co2+:LMA crystal as saturable absorber for a diode-pumped passively Q-switched Nd:YVO4 laser at 1342 nm , 2007 .

[10]  Z. Hussain,et al.  Abrupt onset of a second energy gap at the superconducting transition of underdoped Bi2212 , 2007, Nature.

[11]  T. Togashi,et al.  A versatile system for ultrahigh resolution, low temperature, and polarization dependent laser-angle-resolved photoemission spectroscopy. , 2008, The Review of scientific instruments.

[12]  Lin Zhao,et al.  Coexistence of Fermi arcs and Fermi pockets in a high-Tc copper oxide superconductor , 2009, Nature.

[13]  Y. Chen,et al.  Diode-pumped passively mode-locked 1,342 nm Nd:YVO4 laser with an AlGaInAs quantum-well saturable absorber. , 2009, Optics letters.

[14]  Jianquan Yao,et al.  High-power continuous-wave diode-end-pumped intracavity-frequency-doubled Nd:GdVO4/LBO red laser , 2009 .

[15]  Jingliang He,et al.  Near-diffraction-limited,35.4 W laser-diode end-pumped Nd:YVO4 slab laser operating at 1342 nm. , 2009, Optics letters.

[16]  S. Zhu,et al.  Diode-pumped passively mode-locked Nd:YVO4 laser at 1342 nm with periodically poled LiNbO3. , 2011, Optics letters.

[17]  High-power 880-nm diode-directly-pumped passively mode-locked Nd:YVO₄ laser at 1342 nm with a semiconductor saturable absorber mirror. , 2011, Optics letters.

[18]  J. L’huillier,et al.  888 nm pumped 1342 nm Nd:YVO4 oscillator Kerr-lens mode-locked using cascaded second-order nonlinearities , 2012 .