Author Affiliations
Abstract
1 Kansai Photon Science Institute, National Institutes for Quantum Science and Technology, Kyoto619-0215, Japan
2 Center for Relativistic Laser Science, Institute for Basic Science, Gwangju61005, Republic of Korea
3 Advanced Photonics Research Institute, Gwangju Institute of Science and Technology, Gwangju61005, Republic of Korea
4 Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju61005, Republic of Korea
5 Helmholtz-Zentrum Dresden – Rossendorf, 01328Dresden, Germany
6 Technische Universität Dresden, 01062Dresden, Germany
We report on the design and characterization of the plasma mirror system installed on the J-KAREN-P laser at the Kansai Photon Science Institute, National Institutes for Quantum Science and Technology. The reflectivity of the single plasma mirror system exceeded 80%. In addition, the temporal contrast was improved by two orders of magnitude at 1 ps before the main pulse. Furthermore, the laser near-field spatial distribution after the plasma mirror was kept constant at plasma mirror fluence of less than 100 kJ/cm2. We also present the results of investigating the difference and the fluctuation in energy, pulse width and pointing stability with and without the plasma mirror system.
high-power lasers laser plasma plasma mirror 
High Power Laser Science and Engineering
2022, 10(4): 04000e25
Author Affiliations
Abstract
1 AWE, Aldermaston, Reading, UK
2 OxCHEDS, Clarendon Laboratory, Department of Physics, University of Oxford, Oxford, UK
3 CIFS, Blackett Laboratory, Imperial College, London, UK
4 NIF & Photon Science Directorate, Lawrence Livermore National Laboratory, Livermore, USA
5 Fraunhofer Institute for Laser Technology (ILT), Aachen, Germany
6 Chair for Laser Technology LLT, RWTH Aachen University, Aachen, Germany
7 University of Rochester, Laboratory for Laser Energetics, Rochester, USA
8 Central Laser Facility, STFC Rutherford Appleton Laboratory, Chilton, Didcot, UK
9 LULI, CNRS, CEA, Sorbonne Universités, École Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
10 Department of Physics, The Ohio State University, Columbus, USA
11 Centre for Ultrafast Optical Science, University of Michigan, Ann Arbor, USA
12 Intense Laser Irradiation Laboratory, Istituto Nazionale di Ottica (INO), CNR, Pisa, Italy
13 Institute of Optics and Quantum Electronics, Friedrich-Schiller-University Jena and Helmholtz Institute, Jena, Germany
14 The Graduate School for the Creation of New Photonics Industries, Nishiku, Hamamatsu, Japan
15 Institute of Applied Physics, Russian Academy of Sciences, Nizhny Novgorod, Russia
16 Institute of Laser Engineering, Osaka University, Suita, Osaka, Japan
17 ELI-Beamlines, Institute of Physics, Czech Academy of Sciences, Prague, Czech Republic
18 State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
19 National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
20 Institute for Applied Physics (IAP) at Friedrich-Schiller-University Jena, Jena, Germany
21 Helmholtz Institute Jena, Jena, Germany
22 Fraunhofer Institute for Applied Optics and Precision Engineering (IOF), Jena, Germany
23 Key Laboratory for Laser Plasma (Ministry of Education), School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
24 Centre for Relativistic Laser Science (CoReLS), Institute for Basic Science, Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju, South Korea
25 SUPA, Department of Physics, University of Strathclyde, Glasgow, UK
26 Colorado State University, Fort Collins, Colorado, USA
27 Department of Experimental Physics, University of Szeged, Szeged, Hungary
28 National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
In the 2015 review paper ‘Petawatt Class Lasers Worldwide’ a comprehensive overview of the current status of high-power facilities of ${>}200~\text{TW}$ was presented. This was largely based on facility specifications, with some description of their uses, for instance in fundamental ultra-high-intensity interactions, secondary source generation, and inertial confinement fusion (ICF). With the 2018 Nobel Prize in Physics being awarded to Professors Donna Strickland and Gerard Mourou for the development of the technique of chirped pulse amplification (CPA), which made these lasers possible, we celebrate by providing a comprehensive update of the current status of ultra-high-power lasers and demonstrate how the technology has developed. We are now in the era of multi-petawatt facilities coming online, with 100 PW lasers being proposed and even under construction. In addition to this there is a pull towards development of industrial and multi-disciplinary applications, which demands much higher repetition rates, delivering high-average powers with higher efficiencies and the use of alternative wavelengths: mid-IR facilities. So apart from a comprehensive update of the current global status, we want to look at what technologies are to be deployed to get to these new regimes, and some of the critical issues facing their development.
exawatt lasers high-power lasers petawatt lasers ultra-high intensity 
High Power Laser Science and Engineering
2019, 7(3): 03000e54
Author Affiliations
Abstract
Center for Relativistic Laser Science, Institute for Basic Science (IBS), Gwangju 500-712, Korea
Recently there has been great progress in laser-driven plasma-based accelerators by exploiting high-power lasers, where electron beams can be accelerated to multi-GeV energy in a centimeter-scale plasma due to the laser wakefield acceleration mechanism. While, to date, worldwide research on laser plasma accelerators has been focused on the creation of compact particle and radiation sources for basic sciences, medical and industrial applications, there is great interest in applications for high-energy physics and astrophysics, exploring unprecedented high-energy frontier phenomena. In this context, we present an overview of experimental achievements in laser plasma acceleration from the perspective of the production of GeV-level electron beams, and deduce the scaling formulas capable of predicting experimental results self-consistently, taking into account the propagation of a relativistic laser pulse through plasma and the accelerating field reduction due to beam loading. Finally, we present design examples for 10-GeV-level laser plasma acceleration, which is expected in near-term experiments by means of petawatt-class lasers.
electron beam loading GeV-level electron beam acceleration laser plasma (wakefield) accelerators petawatt-class lasers propagation of relativistic laser pulses in plasma 
High Power Laser Science and Engineering
2015, 3(1): 01000e10

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