Laser Requirements for High-Order Harmonic Generation by Relativistic Plasma Singularities
We discuss requirements on relativistic-irradiance (I0 > 1018 W/cm2) high-power (multi-terawatt) ultrashort (femtosecond) lasers for efficient generation of high-order harmonics in gas jet targets in a new regime discovered recently (Pirozhkov et al., 2012). Here, we present the results of se...
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MDPI AG
2018-03-01
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author | Alexander S. Pirozhkov Timur Zh. Esirkepov Tatiana A. Pikuz Anatoly Ya. Faenov Akito Sagisaka Koichi Ogura Yukio Hayashi Hideyuki Kotaki Eugene N. Ragozin David Neely James K. Koga Yuji Fukuda Masaharu Nishikino Takashi Imazono Noboru Hasegawa Tetsuya Kawachi Hiroyuki Daido Yoshiaki Kato Sergei V. Bulanov Kiminori Kondo Hiromitsu Kiriyama Masaki Kando |
author_facet | Alexander S. Pirozhkov Timur Zh. Esirkepov Tatiana A. Pikuz Anatoly Ya. Faenov Akito Sagisaka Koichi Ogura Yukio Hayashi Hideyuki Kotaki Eugene N. Ragozin David Neely James K. Koga Yuji Fukuda Masaharu Nishikino Takashi Imazono Noboru Hasegawa Tetsuya Kawachi Hiroyuki Daido Yoshiaki Kato Sergei V. Bulanov Kiminori Kondo Hiromitsu Kiriyama Masaki Kando |
author_sort | Alexander S. Pirozhkov |
collection | DOAJ |
description | We discuss requirements on relativistic-irradiance (I0 > 1018 W/cm2) high-power (multi-terawatt) ultrashort (femtosecond) lasers for efficient generation of high-order harmonics in gas jet targets in a new regime discovered recently (Pirozhkov et al., 2012). Here, we present the results of several experimental campaigns performed with different irradiances, analyse the obtained results and derive the required laser parameters. In particular, we found that the root mean square (RMS) wavefront error should be smaller than ~100 nm (~λ/8). Further, the angular dispersion should be kept considerably smaller than the diffraction divergence, i.e., μrad level for 100–300-mm beam diameters. The corresponding angular chirp should not exceed 10−2 μrad/nm for a 40-nm bandwidth. We show the status of the J-KAREN-P laser (Kiriyama et al., 2015; Pirozhkov et al., 2017) and report on the progress towards satisfying these requirements. |
first_indexed | 2024-12-10T19:34:47Z |
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institution | Directory Open Access Journal |
issn | 2412-382X |
language | English |
last_indexed | 2024-12-10T19:34:47Z |
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spelling | doaj.art-0767684262ea428a96515cbae42ac57f2022-12-22T01:36:09ZengMDPI AGQuantum Beam Science2412-382X2018-03-0121710.3390/qubs2010007qubs2010007Laser Requirements for High-Order Harmonic Generation by Relativistic Plasma SingularitiesAlexander S. Pirozhkov0Timur Zh. Esirkepov1Tatiana A. Pikuz2Anatoly Ya. Faenov3Akito Sagisaka4Koichi Ogura5Yukio Hayashi6Hideyuki Kotaki7Eugene N. Ragozin8David Neely9James K. Koga10Yuji Fukuda11Masaharu Nishikino12Takashi Imazono13Noboru Hasegawa14Tetsuya Kawachi15Hiroyuki Daido16Yoshiaki Kato17Sergei V. Bulanov18Kiminori Kondo19Hiromitsu Kiriyama20Masaki Kando21Kansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanGraduate School of Engineering, Osaka University, Suita, Osaka 565-0871, JapanJoint Institute for High Temperatures of the Russian Academy of Sciences, Moscow 125412, RussiaKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanP. N. Lebedev Physical Institute of the Russian Academy of Sciences, Moscow 119991, RussiaCentral Laser Facility, Rutherford Appleton Laboratory, STFC, Oxon OX11 0QX, UKKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanNaraha Remote Technology Development Center, JAEA, Yamadaoka, Naraha, Futaba, Fukushima 979-0513, JapanThe Graduate School for the Creation of New Photonics Industries, Nishiku, Hamamatsu, Shizuoka 431-1202, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanKansai Photon Science Institute (KPSI), National Institutes for Quantum and Radiological Science and Technology (QST), Kizugawa, Kyoto 619-0215, JapanWe discuss requirements on relativistic-irradiance (I0 > 1018 W/cm2) high-power (multi-terawatt) ultrashort (femtosecond) lasers for efficient generation of high-order harmonics in gas jet targets in a new regime discovered recently (Pirozhkov et al., 2012). Here, we present the results of several experimental campaigns performed with different irradiances, analyse the obtained results and derive the required laser parameters. In particular, we found that the root mean square (RMS) wavefront error should be smaller than ~100 nm (~λ/8). Further, the angular dispersion should be kept considerably smaller than the diffraction divergence, i.e., μrad level for 100–300-mm beam diameters. The corresponding angular chirp should not exceed 10−2 μrad/nm for a 40-nm bandwidth. We show the status of the J-KAREN-P laser (Kiriyama et al., 2015; Pirozhkov et al., 2017) and report on the progress towards satisfying these requirements.http://www.mdpi.com/2412-382X/2/1/7high-power femtosecond lasershigh-power laser qualityrelativistic laser plasmarelativistic plasma singularitiescoherent X-ray generationburst intensification by singularity-emitting radiation |
spellingShingle | Alexander S. Pirozhkov Timur Zh. Esirkepov Tatiana A. Pikuz Anatoly Ya. Faenov Akito Sagisaka Koichi Ogura Yukio Hayashi Hideyuki Kotaki Eugene N. Ragozin David Neely James K. Koga Yuji Fukuda Masaharu Nishikino Takashi Imazono Noboru Hasegawa Tetsuya Kawachi Hiroyuki Daido Yoshiaki Kato Sergei V. Bulanov Kiminori Kondo Hiromitsu Kiriyama Masaki Kando Laser Requirements for High-Order Harmonic Generation by Relativistic Plasma Singularities Quantum Beam Science high-power femtosecond lasers high-power laser quality relativistic laser plasma relativistic plasma singularities coherent X-ray generation burst intensification by singularity-emitting radiation |
title | Laser Requirements for High-Order Harmonic Generation by Relativistic Plasma Singularities |
title_full | Laser Requirements for High-Order Harmonic Generation by Relativistic Plasma Singularities |
title_fullStr | Laser Requirements for High-Order Harmonic Generation by Relativistic Plasma Singularities |
title_full_unstemmed | Laser Requirements for High-Order Harmonic Generation by Relativistic Plasma Singularities |
title_short | Laser Requirements for High-Order Harmonic Generation by Relativistic Plasma Singularities |
title_sort | laser requirements for high order harmonic generation by relativistic plasma singularities |
topic | high-power femtosecond lasers high-power laser quality relativistic laser plasma relativistic plasma singularities coherent X-ray generation burst intensification by singularity-emitting radiation |
url | http://www.mdpi.com/2412-382X/2/1/7 |
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