High-flux high-energy ion beam production from stable collisionless shock acceleration by intense petawatt-picosecond laser pulses
A scheme to achieve stable collisionless shock acceleration (CSA) of ions from a near-critical plasma by intense petawatt-picosecond laser pulses is proposed, where the plasma is confined in a high-Z solid tube. The application of the tube, on the one hand, restrains the plasma from transverse therm...
Main Authors: | , , , , , , , , , |
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Format: | Article |
Language: | English |
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IOP Publishing
2019-01-01
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Series: | New Journal of Physics |
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Online Access: | https://doi.org/10.1088/1367-2630/ab0a8c |
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author | H He B Qiao X F Shen W P Yao Y Xie C T Zhou X T He S P Zhu W B Pei S Z Fu |
author_facet | H He B Qiao X F Shen W P Yao Y Xie C T Zhou X T He S P Zhu W B Pei S Z Fu |
author_sort | H He |
collection | DOAJ |
description | A scheme to achieve stable collisionless shock acceleration (CSA) of ions from a near-critical plasma by intense petawatt-picosecond laser pulses is proposed, where the plasma is confined in a high-Z solid tube. The application of the tube, on the one hand, restrains the plasma from transverse thermal expansion, helping to sustain sufficient density steepening required for shock formation and maintenance; on the other hand, due to the induced sheath field along its wall, pinches hot electrons for recirculation near laser axis, aiding to reach efficient plasma heating that is crucial to have a strong shock velocity for ion reflection. Consequently, stable ion CSA can be maintained for picosecond time scales, resulting in production of high-flux high-energy ion beams. Two-dimensional PIC simulations show that proton beams with narrow energy spread between 50 and 80 MeV and high flux with particle number about 10 ^12 are produced by a laser pulse at intensity 8.8 × 10 ^19 W cm ^−2 and duration 1 ps. By extending the pulse duration to 3 ps, over 100 MeV high-flux proton beams are obtained. |
first_indexed | 2024-03-12T16:29:33Z |
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institution | Directory Open Access Journal |
issn | 1367-2630 |
language | English |
last_indexed | 2024-03-12T16:29:33Z |
publishDate | 2019-01-01 |
publisher | IOP Publishing |
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series | New Journal of Physics |
spelling | doaj.art-87efb61ecb7e4519b6bc186487d079792023-08-08T15:34:50ZengIOP PublishingNew Journal of Physics1367-26302019-01-0121303303510.1088/1367-2630/ab0a8cHigh-flux high-energy ion beam production from stable collisionless shock acceleration by intense petawatt-picosecond laser pulsesH He0https://orcid.org/0000-0003-2202-6781B Qiao1https://orcid.org/0000-0001-7174-5577X F Shen2https://orcid.org/0000-0002-3439-8753W P Yao3https://orcid.org/0000-0002-6017-9300Y Xie4C T Zhou5X T He6S P Zhu7W B Pei8S Z Fu9Department of Physics, Fudan University , Shanghai 200433, People’s Republic of China; Shanghai Institute of Laser Plasma , CAEP, Shanghai, 201800, People’s Republic of China; Center for Applied Physics and Technology, HEDPS, SKLNPT, and School of Physics, Peking University , Beijing, 100871, People’s Republic of ChinaCenter for Applied Physics and Technology, HEDPS, SKLNPT, and School of Physics, Peking University , Beijing, 100871, People’s Republic of China; Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University , Shanghai 200240, People’s Republic of China; Center for Advanced Material Diagnostic Technology, Shenzhen Technology University , Shenzhen 518118, People’s Republic of China; Collaborative Innovation Center of Extreme Optics, Shanxi University , Taiyuan, Shanxi 030006, People’s Republic of ChinaCenter for Applied Physics and Technology, HEDPS, SKLNPT, and School of Physics, Peking University , Beijing, 100871, People’s Republic of China; Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University , Shanghai 200240, People’s Republic of ChinaCenter for Applied Physics and Technology, HEDPS, SKLNPT, and School of Physics, Peking University , Beijing, 100871, People’s Republic of China; Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University , Shanghai 200240, People’s Republic of ChinaCenter for Applied Physics and Technology, HEDPS, SKLNPT, and School of Physics, Peking University , Beijing, 100871, People’s Republic of China; Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University , Shanghai 200240, People’s Republic of ChinaCenter for Applied Physics and Technology, HEDPS, SKLNPT, and School of Physics, Peking University , Beijing, 100871, People’s Republic of China; Center for Advanced Material Diagnostic Technology, Shenzhen Technology University , Shenzhen 518118, People’s Republic of ChinaCenter for Applied Physics and Technology, HEDPS, SKLNPT, and School of Physics, Peking University , Beijing, 100871, People’s Republic of China; Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University , Shanghai 200240, People’s Republic of China; Institute of Applied Physics and Computational Mathematics , Beijing 100094, People’s Republic of ChinaInstitute of Applied Physics and Computational Mathematics , Beijing 100094, People’s Republic of China; Graduate School, China Academy of Engineering Physics , Beijing 100088, People’s Republic of ChinaShanghai Institute of Laser Plasma , CAEP, Shanghai, 201800, People’s Republic of ChinaShanghai Institute of Laser Plasma , CAEP, Shanghai, 201800, People’s Republic of ChinaA scheme to achieve stable collisionless shock acceleration (CSA) of ions from a near-critical plasma by intense petawatt-picosecond laser pulses is proposed, where the plasma is confined in a high-Z solid tube. The application of the tube, on the one hand, restrains the plasma from transverse thermal expansion, helping to sustain sufficient density steepening required for shock formation and maintenance; on the other hand, due to the induced sheath field along its wall, pinches hot electrons for recirculation near laser axis, aiding to reach efficient plasma heating that is crucial to have a strong shock velocity for ion reflection. Consequently, stable ion CSA can be maintained for picosecond time scales, resulting in production of high-flux high-energy ion beams. Two-dimensional PIC simulations show that proton beams with narrow energy spread between 50 and 80 MeV and high flux with particle number about 10 ^12 are produced by a laser pulse at intensity 8.8 × 10 ^19 W cm ^−2 and duration 1 ps. By extending the pulse duration to 3 ps, over 100 MeV high-flux proton beams are obtained.https://doi.org/10.1088/1367-2630/ab0a8claser-driven ion accelerationcollisionless shock accelerationhigh-flux high-energy ion beamspetawatt-picosecond laser pulses |
spellingShingle | H He B Qiao X F Shen W P Yao Y Xie C T Zhou X T He S P Zhu W B Pei S Z Fu High-flux high-energy ion beam production from stable collisionless shock acceleration by intense petawatt-picosecond laser pulses New Journal of Physics laser-driven ion acceleration collisionless shock acceleration high-flux high-energy ion beams petawatt-picosecond laser pulses |
title | High-flux high-energy ion beam production from stable collisionless shock acceleration by intense petawatt-picosecond laser pulses |
title_full | High-flux high-energy ion beam production from stable collisionless shock acceleration by intense petawatt-picosecond laser pulses |
title_fullStr | High-flux high-energy ion beam production from stable collisionless shock acceleration by intense petawatt-picosecond laser pulses |
title_full_unstemmed | High-flux high-energy ion beam production from stable collisionless shock acceleration by intense petawatt-picosecond laser pulses |
title_short | High-flux high-energy ion beam production from stable collisionless shock acceleration by intense petawatt-picosecond laser pulses |
title_sort | high flux high energy ion beam production from stable collisionless shock acceleration by intense petawatt picosecond laser pulses |
topic | laser-driven ion acceleration collisionless shock acceleration high-flux high-energy ion beams petawatt-picosecond laser pulses |
url | https://doi.org/10.1088/1367-2630/ab0a8c |
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