Microchip laser operating at 1338 nm

Q-switched microchip laser emitting radiation at wavelength 1338 nm was designed and realized. This laser was based on monolith crystal which combines in one piece a cooling undoped part (undoped YAG crystal, 4 mm long), active laser part (YAG crystal doped with Nd3+ ions, 12 mm long) and saturable absorber (YAG crystal doped with V3+ ions, 0.7 mm long). The diameter of the diffusion bounded monolith was 5 mm. The initial transmission of the V:YAG part was 85 %. The microchip resonator consists of dielectric mirrors directly deposited on the monolith surfaces. The pump mirror (HT for pump radiation, HR for generated radiation) was placed on the undoped YAG part. The output coupler with reflection 90 % for the generated wavelength was placed on the V3+-doped part. Q-switched microchip laser was tested under pulsed, and CW diode pumping. The pulse length it was the same for all regimes equal to 6.2 ns. The wavelength of linearly polarized laser emission was fixed to 1338 nm. The pulse energy depends on the mean pump power. For pulsed pumping the output pulse energy was stable up to mean pump power 1 W and it was equal to 135 μJ, which corresponds to peak power 22 kW. In CW regime for pumping up to 14 W the pulse energy was stabilized to 37 μJ (peak power 6 kW). The mean output power increased up to 0.4 W only by increase of the generated pulse repetition rate (11 kHz for mean pump power 14 W).

[1]  Helena Jelínková,et al.  Thermal properties of Nd:YAG: Composite active media in a diode-pumped laser , 2003 .

[2]  Krzysztof Kopczynski,et al.  Diode pumped Nd:YVO4 laser at 1.34 μm Q-switched and mode locked by a V3+:YAG saturable absorber , 2001 .

[3]  Alexander M. Malyarevich,et al.  V:YAG – a new passive Q-switch for diode-pumped solid-state lasers , 1998 .

[4]  Krzysztof Kopczynski,et al.  Application of V3+:YAG crystals for Q-switching and mode-locking of 1.3-μm diode-pumped neodymium lasers , 2001 .

[5]  Zeev Burshtein,et al.  Passive Q-switching in Nd:YAG/Cr4+:YAG monolithic microchip laser , 2003 .

[6]  J. J. Zayhowski Microchip lasers , 1997, CLEO '97., Summaries of Papers Presented at the Conference on Lasers and Electro-Optics.

[7]  Konstantin V. Yumashev,et al.  Optical absorption and nonlinear transmission of tetrahedral V3+ (d2) in yttrium aluminum garnet , 1993 .

[8]  Michal Nemec,et al.  V:YAG saturable absorber for flash-lamp and diode-pumped solid state lasers , 2004, SPIE Photonics Europe.

[9]  G. Huber,et al.  Spectroscopy of tetrahedrally coordinated V3+ in oxide crystals , 1998 .

[10]  Helena Jelinkova,et al.  Passively mode-locked Q-switched Nd:YAP 1.34-um/1.08-um laser with efficient hollow-waveguide radiation delivery , 2002, SPIE LASE.

[11]  K. K. Lee,et al.  Self-Q-switched diode-end-pumped Cr,Nd:YAG laser with polarized output. , 1993, Optics letters.

[12]  Humio Inaba,et al.  Analytical and experimental studies on the characteristics of composite solid-state laser rods in diode-end-pumped geometry , 1997 .

[13]  J. Zayhowski,et al.  Single-frequency microchip Nd lasers. , 1989, Optics letters.

[14]  Konstantin V. Yumashev,et al.  Mode-Locking of Near Infrared Lasers with V3+ : YAG Crystal as a Saturable Absorber , 1993 .

[15]  Z. Frukacz,et al.  YAG:V³⁺ : new passive Q-switch for lasers generating radiation within near infrared range , 2000 .

[16]  Engin Molva,et al.  Microchip lasers and their applications in optical microsystems , 1999 .