Petawatt and exawatt class lasers worldwide
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-in...
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Published in | High power laser science and engineering Vol. 7 |
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Main Authors | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
Shanghi
Cambridge University Press
2019
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Subjects | |
Online Access | Get full text |
ISSN | 2095-4719 2052-3289 |
DOI | 10.1017/hpl.2019.36 |
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Abstract | 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. |
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AbstractList | 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. 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. In the 2015 review paper 'Petawatt Class Lasers Worldwide' a comprehensive overview of the current status of highpower facilities of >200 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 multidisciplinary 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. |
ArticleNumber | e54 |
Author | Papadopoulos, Dimitrios Trines, Raoul M. G. M. Penman, Rory R. Hopps, Nicholas W. Shaykin, Andrey A. Spindloe, Christopher Butcher, Thomas Chanteloup, Jean-Christophe F. Qian, Liejia Ma, Jingui Galvanauskas, Almantas Haefner, Constantin Danson, Colin N. Gizzi, Leonida A. Hein, Joachim Kato, Yoshiaki Li, Yutong Szatmári, Sándor Kodama, Ryosuke Limpert, Jens Rocca, Jorge J. Zhu, Jianqiang Nam, Chang Hee Siders, Craig W. Chowdhury, Enam A. Hillier, David I. Korn, Georg Zhu, Ping Khazanov, Efim A. Zuegel, Jonathan D. Li, Ruxin Bromage, Jake Neely, David |
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BackLink | https://hal.science/hal-03037682$$DView record in HAL |
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Keywords | exawatt lasers high-power lasers petawatt lasers ultra-high intensity |
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8599 Danson (S2095471919000367_r35) 1998; 45 Smith (S2095471919000367_r228) 2011; 19 S2095471919000367_r350 S2095471919000367_r355 S2095471919000367_r234 S2095471919000367_r113 S2095471919000367_r356 S2095471919000367_r235 S2095471919000367_r114 S2095471919000367_r357 S2095471919000367_r236 S2095471919000367_r115 S2095471919000367_r237 S2095471919000367_r351 S2095471919000367_r230 S2095471919000367_r352 S2095471919000367_r110 S2095471919000367_r232 S2095471919000367_r353 S2095471919000367_r354 S2095471919000367_r233 S2095471919000367_r112 S2095471919000367_r319 S2095471919000367_r315 S2095471919000367_r316 S2095471919000367_r317 S2095471919000367_r201 S2095471919000367_r322 S2095471919000367_r202 S2095471919000367_r323 S2095471919000367_r324 S2095471919000367_r203 S2095471919000367_r325 S2095471919000367_r204 S2095471919000367_r320 S2095471919000367_r321 S2095471919000367_r200 S2095471919000367_r209 S2095471919000367_r326 Mueller (S2095471919000367_r231) 2018; 10512 S2095471919000367_r205 S2095471919000367_r206 S2095471919000367_r207 S2095471919000367_r329 S2095471919000367_r208 S2095471919000367_r333 S2095471919000367_r212 S2095471919000367_r334 S2095471919000367_r213 S2095471919000367_r214 S2095471919000367_r336 S2095471919000367_r215 S2095471919000367_r330 S2095471919000367_r331 S2095471919000367_r332 S2095471919000367_r211 S2095471919000367_r66 S2095471919000367_r64 S2095471919000367_r62 Xu (S2095471919000367_r126) 2013; 38 S2095471919000367_r61 S2095471919000367_r60 S2095471919000367_r300 S2095471919000367_r301 S2095471919000367_r302 S2095471919000367_r303 Gaul (S2095471919000367_r304) 2016; 717 S2095471919000367_r69 S2095471919000367_r68 S2095471919000367_r67 S2095471919000367_r308 S2095471919000367_r309 S2095471919000367_r305 S2095471919000367_r306 S2095471919000367_r307 Stark (S2095471919000367_r249) 2019; 10897 S2095471919000367_r55 S2095471919000367_r54 S2095471919000367_r52 S2095471919000367_r51 S2095471919000367_r50 Palastro (S2095471919000367_r338) 2015; 22 S2095471919000367_r311 S2095471919000367_r312 S2095471919000367_r313 S2095471919000367_r314 S2095471919000367_r59 Liang (S2095471919000367_r122) 2007; 15 S2095471919000367_r58 S2095471919000367_r56 S2095471919000367_r87 S2095471919000367_r86 S2095471919000367_r85 S2095471919000367_r81 Walker (S2095471919000367_r116) 2017; 874 Ginzburg (S2095471919000367_r172) 2019 S2095471919000367_r77 S2095471919000367_r76 S2095471919000367_r71 S2095471919000367_r70 Tang (S2095471919000367_r256) 2018; 10 S2095471919000367_r78 Bolton (S2095471919000367_r361) 2014; 30 Pogorelsky (S2095471919000367_r281) 2017; 1812 Downer (S2095471919000367_r365) 2013 S2095471919000367_r91 S2095471919000367_r99 S2095471919000367_r98 Roso (S2095471919000367_r111) 2011; 8001 S2095471919000367_r97 S2095471919000367_r96 S2095471919000367_r95 Ebrardt (S2095471919000367_r89) 2010; 244 S2095471919000367_r94 S2095471919000367_r93 S2095471919000367_r92 Barty (S2095471919000367_r178) 2016; 717 |
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Snippet | 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... 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... In the 2015 review paper 'Petawatt Class Lasers Worldwide' a comprehensive overview of the current status of highpower facilities of >200 TW was presented.... |
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SubjectTerms | Bandwidths High power lasers Inertial confinement fusion Laboratories Lasers Optics Physics Power |
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Title | Petawatt and exawatt class lasers worldwide |
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