Neodymium glass laser with a phase conjugate mirror producing 220 J pulses at 0.02 Hz repetition rate.

For pumping multipetawatt Ti:sapphire laser facilities we developed a compact repetitively pulsed laser based on neodymium phosphate glass with pulse energy of 220 J, pulse repetition rate of 0.02 Hz, beam diameter of 43 mm, aperture fill factor of 0.8, and FWHM pulse duration of 30 ns. The phase distortions of laser radiation were compensated by optical phase conjugation via stimulated Brillouin scattering. The depolarization was reduced to 0.4% using linear compensation methods. The beam quality was 2.5 x diffraction limit (150 µrad).

[1]  E. Khazanov,et al.  A two-channel repetitively pulsed Nd:YAG laser operating at 25 Hz with diffraction-limited beam quality , 1999 .

[2]  J.-P. Chambaret,et al.  Extreme light infrastructure: laser architecture and major challenges , 2010, Photonics Europe.

[3]  E. Khazanov,et al.  Simple method of measurement of phase distortions in laser amplifiers , 2012 .

[4]  E. Khazanov,et al.  Neodymium glass laser with a pulse energy of and a pulse repetition rate of , 2013 .

[5]  A. V. Charukhchev,et al.  Laser amplifier based on a neodymium glass rod in diameter , 2014 .

[6]  J. W. Yoon,et al.  Generation of high-contrast, 30 fs, 1.5 PW laser pulses , 2012, 2013 Conference on Lasers and Electro-Optics Pacific Rim (CLEOPR).

[7]  Gerard Mourou,et al.  Quasi-flat-top frequency-doubled Nd:glass laser for pumping of high-power Ti:sapphire amplifiers at a 0.1 Hz repetition rate. , 2008 .

[8]  E. Khazanov,et al.  Large-aperture Nd:glass laser amplifiers with high pulse repetition rate. , 2011, Optics express.

[9]  E. Khazanov,et al.  Investigation of distortions of the laser pulse profile in multipass amplifiers with a stimulated-Brillouin-scattering mirror , 1998 .

[10]  Sargent Jw,et al.  Properties of perfluorinated liquids. , 1970 .

[11]  Bruce W. Shore,et al.  Petawatt laser system , 1997, Other Conferences.

[12]  E. G. Pivinskii,et al.  Generation of picosecond pulses with the wavelength 1.54 μm by two-stage compression in stimulated scattering of nanosecond Nd3+ : YAG laser pulses , 1997 .

[13]  E. Khazanov,et al.  Repetitively pulsed regime of Nd : glass large-aperture laser amplifiers , 2012 .

[14]  Vladislav Ginzburg,et al.  Compact 0.56 Petawatt laser system based on optical parametric chirped pulse amplification in KD*P crystals , 2007 .

[15]  E. Khazanov,et al.  Review of Faraday Isolators for Kilowatt Average Power Lasers , 2014, IEEE Journal of Quantum Electronics.

[16]  Marco Galimberti,et al.  The Vulcan 10 PW project , 2010 .

[17]  K Yamakawa,et al.  0.85-PW, 33-fs Ti:sapphire laser. , 2003, Optics letters.

[18]  Gerard Mourou,et al.  Apollon-10P: Status and implementation , 2012 .

[19]  K. Kokh,et al.  Growth of high quality large size LBO crystals for high energy second harmonic generation , 2010 .

[20]  G. A. Pasmanik,et al.  SBS of repetitively pulsed radiation and possibility of increasing the pump average power , 1995, Other Conferences.

[21]  M. Siegrist Cusp shape reflectors to pump disk or slab lasers. , 1976, Applied optics.

[22]  H. Fujita,et al.  Heavy fluorocarbon liquids for a phase-conjugated stimulated Brillouin scattering mirror. , 1997, Applied optics.

[23]  Gerard Mourou,et al.  Compression of amplified chirped optical pulses , 1985 .

[24]  E. Khazanov,et al.  Compact neodymium phosphate glass laser emitting 100-J, 100-GW pulses for pumping a parametric amplifier of chirped pulses , 2005 .

[25]  Hisanori Fujita,et al.  Very high energy SBS phase conjugation and pulse compression in fluorocarbon liquids , 2000, Advanced High-Power Lasers and Applications.

[26]  D. Hanna,et al.  Performance of a Nd: YAG oscillator/ampflifier with phase-conjugation via stimulated Brillouin scattering , 1985 .

[27]  E. Khazanov,et al.  Four-pass Nd:YAG laser system with compensation of aberration and polarisation distortions of the wavefront , 1996 .