Method to improve beam quality by compensating spherical aberrations in master oscillator power amplifier laser systems.

A method is presented for beam quality improvement, in master oscillator power amplifier laser systems. Intensive study was first carried out with the beam wavefront evolution in a laser resonator. When the laser beam propagates inside the resonator, the spherical aberration coefficient of the beam wavefront can change sign, i.e., the negative spherical aberration coefficient can turn to positive, and vice versa. This process also occurs when the beam propagates outside the resonator in a free space. The laser beam, from an oscillator with negative spherical aberration, was found to be well-compensated by the positive spherical aberration of a strongly pumped laser rod in a laser amplifier. The laser beam quality M2 factor has been significantly improved, from 2.2 to 1.4, while the output power has been scaled from 31 W up to 60 W.

[1]  Suwas Nikumb,et al.  Further development of a diode-pumped Nd:YVO4/Nd:YAG hybrid oscillator , 1998, Other Conferences.

[2]  Volker Wulfmeyer,et al.  Diode-pumped Nd:YAG master oscillator power amplifier with high pulse energy, excellent beam quality, and frequency-stabilized master oscillator as a basis for a next-generation lidar system. , 2005, Applied optics.

[3]  Zhigang Zhao,et al.  Beam Profile Evolution and Beam Quality Changes Inside a Diode-End-Pumped Laser Oscillator , 2014, IEEE Journal of Quantum Electronics.

[4]  S. Jackel,et al.  Correction of spherical and azimuthal aberrations in radially polarized beams from strongly pumped laser rods. , 2005, Applied optics.

[5]  David C. Brown Nonlinear thermal distortion in YAG rod amplifiers , 1998 .

[6]  B. Neubert,et al.  Influences on the beam propagation ratio M2 , 2005 .

[7]  J. Y. Wang,et al.  Wave-front interpretation with Zernike polynomials. , 1980, Applied optics.

[8]  P.-Y. Thro,et al.  Novel method to improve the performance of Nd:YAG high-power low-divergence lasers using a passive compensation of the spherical aberration inside the resonator , 2005, SPIE LASE.

[9]  T. Riesbeck,et al.  Influence of spherical aberrations on the performance of dynamically stable resonators , 2008 .

[10]  Anthony E. Siegman,et al.  New developments in laser resonators , 1990, Photonics West - Lasers and Applications in Science and Engineering.

[11]  TEM 00 enhancement in CW Nd-YAG by thermal lensing compensation , 1971 .

[12]  Y. Lumer,et al.  Use of phase corrector plates to increase the power of radially polarized oscillators , 2010 .

[13]  I. Buske,et al.  Diffraction analysis of aberrated laser resonators , 2006 .

[14]  N. Hodgson,et al.  Influence of spherical aberration of the active medium on the performance of Nd:YAG lasers , 1993 .

[15]  J. Bourderionnet,et al.  Influence of aberrations on fundamental mode of high power rod solid-state lasers , 2002 .

[16]  A J Alcock,et al.  High-efficiency diode-pumped Nd:YVO(4) slab laser. , 1993, Optics letters.

[18]  S. Jackel,et al.  Elimination of Spherical Aberration in Multi-kW, Nd:YAG, Rod Pump-Chambers by Pump-Distribution Control , 2005 .

[19]  M. Gilbert,et al.  Thermal lensing and spherical aberration in high-power transversally pumped laser rods , 2006 .

[20]  Jun Chen,et al.  Influences of spherical aberration on resonator's stable zones and fundamental mode output power scaling of solid state laser oscillators. , 2012, Optics express.

[21]  J J Kasinski,et al.  Near-diffraction-limited, high-energy, high-power, diode-pumped laser using thermal aberration correction with aspheric diamond-turned optics. , 1996, Applied optics.

[22]  A. Siegman,et al.  Analysis of laser beam quality degradation caused by quartic phase aberrations. , 1993, Applied optics.

[23]  Rosario Martínez-Herrero,et al.  Beam-quality changes generated by thermally-induced spherical aberration in laser cavities , 1995 .