Laser Technology Development for High Peak Power Lasers Achieving Kilowatt Average Power and Beyond

Novel architectures of Petawatt-class, high peak power laser systems that allow operating at high repetition rates are opening a new arena of commercial applications of secondary sources and discovery science. The natural path to higher average power is the reduction of the total heat load induced and generated in the laser gain medium and eliminating other inefficiencies with the goal to turn more energy into laser photons while maintaining good beam quality. However, the laser architecture must be tailored to the specific application and laser parameters such as wavelength, peak power and intensity, pulse length, and shot rate must be optimized. We have developed a number of different concepts tailored to secondary source generation that minimize inefficiencies and maximize the average power. The Scalable Highaverage- power Advanced Radiographic Capability (SHARC) and the Big Aperture Thulium (BAT) laser are examples of two such high average power laser concepts; SHARC is designed for production of ion beams and x-rays, and exploration of high energy density physics at 1.5 kW average power, and BAT is envisioned for driving laser-based electron accelerators at 300 kW average power.

[1]  Christophe Szwaj,et al.  Horizon 2020 EuPRAXIA design study , 2017 .

[2]  K. Nakamura,et al.  Multi-GeV electron beams from capillary-discharge-guided subpetawatt laser pulses in the self-trapping regime. , 2014, Physical review letters.

[3]  Jay W. Dawson,et al.  Performance measurements of the injection laser system configured for picosecond scale advanced radiographic capability , 2010 .

[4]  David Neely,et al.  Laser-driven x-ray and neutron source development for industrial applications of plasma accelerators , 2015 .

[5]  B. Samson,et al.  Tm-Doped Fiber Lasers: Fundamentals and Power Scaling , 2009, IEEE Journal of Selected Topics in Quantum Electronics.

[6]  H T Powell,et al.  Petawatt laser pulses. , 1999, Optics letters.

[7]  C. D. Marshall,et al.  Next-generation laser for Inertial Confinement Fusion , 1998 .

[8]  J. A. Britten,et al.  A compressor for high average power ultrafast laser pulses with high energies , 2017, 2017 Conference on Lasers and Electro-Optics (CLEO).

[9]  D. Kramer,et al.  Hybrid OPCPA/Glass 10 PW laser at 1 shot a minute , 2018, 2018 Conference on Lasers and Electro-Optics (CLEO).

[10]  V. Leroux,et al.  Lux – A laser–plasma driven undulator beamline , 2018, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment.

[11]  Patrick Georges,et al.  The Apollon 10 PW laser: experimental and theoretical investigation of the temporal characteristics , 2016, High Power Laser Science and Engineering.

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

[13]  A. Erlandson,et al.  High average power, diode pumped petawatt laser systems: a new generation of lasers enabling precision science and commercial applications , 2017, Optics + Optoelectronics.

[14]  J. Piper,et al.  Spectroscopy, modeling, and laser operation of thulium-doped crystals at 2.3 /spl mu/m , 2000, IEEE Journal of Quantum Electronics.

[15]  Antonio Lucianetti,et al.  Kilowatt average power 100 J-level diode pumped solid state laser , 2017 .

[16]  Yuxin Leng,et al.  339  J high-energy Ti:sapphire chirped-pulse amplifier for 10  PW laser facility. , 2018, Optics letters.

[17]  Yuxin Leng,et al.  High-energy large-aperture Ti:sapphire amplifier for 5 PW laser pulses. , 2015, Optics letters.

[18]  W. P. Leemans BELLA LASER AND OPERATIONS* , 2013 .

[19]  Colin N. Danson,et al.  Petawatt class lasers worldwide , 2015, High Power Laser Science and Engineering.

[20]  A C Erlandson,et al.  Optical properties of turbulent channel flow. , 1990, Applied optics.

[21]  Andy J. Bayramian,et al.  Nd:Glass Laser Design for Laser ICF Fission Energy (LIFE) , 2009 .

[22]  Lloyd L. Chase,et al.  Infrared cross-section measurements for crystals doped with Er/sup 3+/, Tm/sup 3+/, and Ho/sup 3+/ , 1992 .

[23]  Andrea Favalli,et al.  Neutron imaging with the short-pulse laser driven neutron source at the Trident laser facility , 2016 .

[24]  Eric Esarey,et al.  Design considerations for a laser-plasma linear collider , 2009 .

[25]  Yong Wang,et al.  0.85  PW laser operation at 3.3  Hz and high-contrast ultrahigh-intensity λ = 400  nm second-harmonic beamline. , 2017, Optics letters.

[26]  Junji Kawanaka,et al.  High Power Lasers and Their New Applications , 2008 .

[27]  Jin Woo Yoon,et al.  4.2  PW, 20  fs Ti:sapphire laser at 0.1  Hz. , 2017, Optics letters.

[28]  Nicolas Bonod,et al.  Diffraction gratings: from principles to applications in high-intensity lasers , 2016 .

[29]  Hoang T. Nguyen,et al.  Active cooling of pulse compression diffraction gratings for high energy, high average power ultrafast lasers. , 2016, Optics express.

[30]  G. F. Albrecht,et al.  Flow, Heat Transfer, And Wavefront Distortion In A Gas Cooled Disk Amplifier , 1989, Photonics West - Lasers and Applications in Science and Engineering.

[31]  Kiminori Kondo,et al.  High-contrast high-intensity repetitive petawatt laser. , 2018, Optics letters.

[32]  S. Laux,et al.  Latest results of 10 petawatt laser beamline for ELi nuclear physics infrastructure , 2016, SPIE LASE.

[33]  Gabe Guss,et al.  Picosecond laser damage performance assessment of multilayer dielectric gratings in vacuum. , 2015, Optics express.

[34]  Marco Borghesi,et al.  Recent advances in laser-driven neutron sources , 2016 .

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

[36]  Hoang T. Nguyen,et al.  Low-dispersion low-loss dielectric gratings for efficient ultrafast laser pulse compression at high average powers , 2018, Optics & Laser Technology.

[37]  Andy J. Bayramian,et al.  The Mercury Project: A High Average Power, Gas-Cooled Laser for Inertial Fusion Energy Development , 2007 .

[38]  Walter Koechner,et al.  Solid-State Laser Engineering , 1976 .

[39]  Robert L. Kustom An Overview of the Spallation Neutron Source Project , 2000 .

[40]  Todd Ditmire,et al.  The Science and Applications of Ultrafast, Ultraintense Lasers: Opportunities in science and technology using the brightest light known to man; a report on the SAUUL workshop held June 17-19, 2002 , 2002 .

[41]  Andy J. Bayramian,et al.  Comparison of Nd:phosphate glass, Yb:YAG and Yb:S-FAP laser beamlines for laser inertial fusion energy (LIFE) [Invited] , 2011 .

[42]  Элвин С. Эрландсон Spatial filters for high average power lasers , 2010 .