Near forward scattering light of planar film target driven by broadband laser

Long Xin-Yu; Wang Pei-Pei; An Hong-Hai; Xiong Jun; Xie Zhi-Yong; Fang Zhi-Heng; Sun Jin-Ren; Wang Chen

doi:10.7498/aps.73.20231613

Abstract

Laser plasma interaction (LPI) has always been an important research topic in the ignition phase of inertial confinement fusion (ICF). Over the years, researchers have attempted to use various laser beam smoothing schemes and optimized light source solutions to suppress the development of LPI. Among them, low-coherence laser drivers have attracted widespread attention in the fields of laser-plasma physics and laser technology in recent years. Recently, a broadband second harmonic laser facility named “Kunwu” has provided a reliable experimental research platform for the LPI process driven by broadband lasers. Aiming at the strong stimulated Brillouin scattering (SBS) and stimulated Raman scattering (SRS) in the LPI process of large-scale low-density plasma, forward scattering experiment and near-forward scattering experiment on C₈H₈ planar film targets driven by broadband laser and narrowband laser under the same conditions are carried out. Based on the “Kunwu” laser facility, two sets of measurement systems are designed, one is centered around fiber-heads and spectrometer, and the other around phototubes and oscilloscope. These systems enable multi-directional precise measurements of scattered lightand a comprehensive analysis of LPI. The main focus is on the comparison of the components and spectral information of the scattering beams between broadband laser and narrowband laser, and it is found that the LPI processes driven by broadband laser and narrowband laser are greatly different. Additionally, preliminary results indicate that broadband laser exhibits a stronger penetration capability than narrowband laser. The time to ablation the target and penetrate the plasma are both nearly 1 ns ahead, with the transmitted energy increased by nearly an order of magnitude. And after penetrating the plasma, there is a smaller spatial divergence angle. These results provide good reference value for better understanding the effect of broadband laser on LPI.

Keywords:

Authors and contacts

Shanghai Institute of Laser Plasma, China Academy of Engineering Physics, Shanghai 201800, China

Corresponding author: Sun Jin-Ren, sunjinren@263.net ; Wang Chen, wangch@mail.shcnc.ac.cn

Funds: Project supported by the National Natural Science Foundation of China (Grant Nos. 12074353, 12075227).

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References

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[23]	Gao Y, Cui Y, Ji L, Rao D, Zhao X, Li F, Liu D, Feng W, Xia L, Liu J 2020 Matter Radiat. Extremes 5 065201 Google Scholar
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[25]	Lei A, Kang N, Zhao Y, Liu H, An H, Xiong J, Wang R, Xie Z, Tu Y, Xu G, Zhou X, Fang Z, Wang W, Xia L, Feng W, Zhao X, Ji L, Cui Y, Zhou S, Liu Z, Zheng C, Wang L, Gao Y, Huang X, Fu S 2024 Phys. Rev. Lett. 132 035102 Google Scholar
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[27]	Moody J, Williams E, Glenzer S, Young P, Hawreliak J, Gouveia A, Wark J 2003 Phys. Rev. Lett. 90 245001 Google Scholar
[28]	Froula D, Divol L, Meezan N, Dixit S, Neumayer P, Moody J, Pollock B, Ross J, Suter L, Glenzer S 2007 Phys. Plasmas 14 055705 Google Scholar
[29]	Moody J, MacGowan B, Glenzer S, Kirkwood R, Kruer W, Montgomery D, Schmitt A, Williams E, Stone G 2000 Phys. Plasmas 7 2114 Google Scholar

Cited By

图 1 实验方案示意图

Figure 1. Sketch of the experimental setup.

DownLoad: Full-Size Img PowerPoint

图 2 靶室内部探测器结构示意图

Figure 2. Schematic diagram of the detector inside target chamber.

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图 3 通过漫反射板系统测量的前向光信号积分光谱

Figure 3. Integrated spectrum of forward light measured by diffuse reflector system.

DownLoad: Full-Size Img PowerPoint

图 4 前向透过激光能量的时间特性

Figure 4. Temporal characteristics of transmitted light.

DownLoad: Full-Size Img PowerPoint

图 5 位于20°位置的L2探测器测量得到的大角度近前向散射积分光谱

Figure 5. Integrated spectrum of large-angle near-forward scattering light measured by L2 detector located at 20°.

DownLoad: Full-Size Img PowerPoint

图 6 窄带与宽带激光驱动条件下不同角度的大角度近前向散射能量份额　(a) SBS; (b) SRS

Figure 6. Share of large-angle near-forward scattering light at different angles driven by boardband and narrowband laser: (a) SBS signals; (b) SRS signals.

DownLoad: Full-Size Img PowerPoint

图 7 近前向散射能量与透过激光能量的比值　(a) SBS; (b) SRS

Figure 7. Ratio of near-forward scattering energy to transmitted laser energy: (a) SBS signals; (b) SRS signals.

DownLoad: Full-Size Img PowerPoint

图 8 透过激光的能量弥散示意图

Figure 8. Schematic diagram of transmitted beam spray.

DownLoad: Full-Size Img PowerPoint

表 1 驱动10 μm厚C₈H₈靶的透过激光能量

Table 1. Transmitted laser energy driving a 10 μm thick C₈H₈ target.

序号	带宽	激光能量/J	卡计能量/J	标定后能量/J	透过能量百分比/%
1	宽带	680	172.8	138.6	20.4
2	宽带	685	152.0	121.9	17.8
3	窄带	694	16.9	13.3	1.9
4	窄带	694	13.7	10.8	1.6
5	窄带	608	13.1	10.3	1.7

DownLoad: CSV

[1]	吴钟书, 赵耀, 翁苏明, 陈民, 盛政明 2019 物理学报 68 195202 Google Scholar Wu Charles F, Zhao Y, Weng S M, Chen M, Sheng Z M 2019 Acta Phys. Sin. 68 195202 Google Scholar
[2]	Seaton A, Arber T 2020 Phys. Plasmas 27 082704 Google Scholar
[3]	Myatt J, Zhang J, Short R, Maximov A, Seka W, Froula D, Edgell D, Michel D, Igumenshchev I, Hinkel D 2014 Phys. Plasmas 21 055501 Google Scholar
[4]	Pak A, Divol L, Kritcher A, Ma T, Ralph J, Bachmann B, Benedetti L, Casey D, Celliers P, Dewald E 2017 Phys. Plasmas 24 056306 Google Scholar
[5]	Lushnikov P M, Rose H A 2006 Plasma Phys. Controlled Fusion 48 1501 Google Scholar
[6]	Edwards M, Patel P, Lindl J, Atherton L, Glenzer S, Haan S, Kilkenny J, Landen O, Moses E, Nikroo A 2013 Phys. Plasmas 20 070501 Google Scholar
[7]	Turnbull D, Michel P, Ralph J, Divol L, Ross J, Hopkins L B, Kritcher A, Hinkel D, Moody J 2015 Phys. Rev. Lett. 114 125001 Google Scholar
[8]	Li C, Dong L, Feng J, Huang Y, Sun H 2020 Rev. Sci Instrum. 91 026105 Google Scholar
[9]	Froula D, Divol L, London R, Berger R, Döppner T, Meezan N, Ross J, Suter L, Sorce C, Glenzer S 2009 Phys. Rev. Lett. 103 045006 Google Scholar
[10]	Niemann C, Berger R, Divol L, Kirkwood R, Moody J, Sorce C, Glenzer S 2011 J. Instrum. 6 P10008 Google Scholar
[11]	Ruyer C, Debayle A, Loiseau P, Masson-Laborde P, Fuchs J, Casanova M, Marquès J, Romagnani L, Antici P, Bourgeois N 2021 Phys. Plasmas 28 052701 Google Scholar
[12]	Michel P, Rosenberg M, Seka W, Solodov A, Short R, Chapman T, Goyon C, Lemos N, Hohenberger M, Moody J 2019 Phys. Rev. E 99 033203 Google Scholar
[13]	余诗瀚, 李晓锋, 翁苏明, 赵耀, 马行行, 陈民, 盛政明 2021 强激光与粒子束 33 012006 Google Scholar Yu S H, Li X F, Weng S M, Zhao Y, Ma H H, Chen M, Sheng Z M 2021 High Power Laser Part. Beams 33 012006 Google Scholar
[14]	Duluc M, Penninckx D, Loiseau P, Riazuelo G, Bourgeade A, Chatagnier A, d'Humières E 2019 Phys. Plasmas 26 42707 Google Scholar
[15]	Sarri G, Cecchetti C, Jung R, Hobbs P, James S, Lockyear J, Stevenson R, Doria D, Hoarty D, Willi O 2011 Phys. Rev. Lett. 106 095001 Google Scholar
[16]	杨冬, 李志超, 李三伟, 郝亮, 李欣, 郭亮, 邹士阳, 蒋小华, 彭晓世, 徐涛, 理玉龙, 郑春阳, 蔡洪波, 刘占军, 郑坚, 龙韬, 王哲斌, 黎航, 况龙钰, 李琦, 王峰, 刘慎业, 杨家敏, 江少恩, 张保汉, 丁永坤 2018 中国科学: 物理学, 力学, 天文学 48 065203 Google Scholar Yang D, Li Z C, Li S W, Hao L, Li X, Guo L, Zou S Y, Jiang X H, Peng X S, Xu T, Li Y L, Zheng C Y, Cai H B, Liu Z J, Zheng J, Long T, Wang Z B, Li H, Kuang Y L, Li Q, Wang F, Liu S Y, Yang J M, Jiang S E, Zhang B H, Ding Y K 2018 Sci. Sin-Phys. Mech. Astron. 48 065203 Google Scholar
[17]	赵耀, 郑君, 於陆勒, 陈民, 翁苏明, 盛政明 2015 中国科学: 物理学, 力学, 天文学 45 035201 Google Scholar Zhao Y, Zheng J, Yu L Q, Chen M, Weng S M, Sheng Z M 2015 Sci. Sin-Phys. Mech. Astron. 45 035201 Google Scholar
[18]	Zhao Y, Weng S, Chen M, Zheng J, Zhuo H, Ren C, Sheng Z, Zhang J 2017 Phys. Plasmas 24 112102 Google Scholar
[19]	Zhao Y, Weng S, Sheng Z, Zhu J 2019 Plasma Phys. Controlled Fusion 61 115008 Google Scholar
[20]	Zhou H, Xiao C, Zou D, Li X, Yin Y, Shao F, Zhuo H 2018 Phys. Plasmas 25 062703 Google Scholar
[21]	Bates J, Follett R, Shaw J, Obenschain S, Myatt J, Weaver J, Wolford M, Kehne D, Myers M, Kessler T 2023 Phys. Plasmas 30 052703 Google Scholar
[22]	刘庆康, 张旭, 蔡洪波, 张恩浩, 高妍琦, 朱少平 2024 物理学报 73 055202 Google Scholar Liu Q K, Zhang X, Cai H B, Zhang E H, Gao Y Q, Zhu S P 2024 Acta Phys. Sin. 73 055202 Google Scholar
[23]	Gao Y, Cui Y, Ji L, Rao D, Zhao X, Li F, Liu D, Feng W, Xia L, Liu J 2020 Matter Radiat. Extremes 5 065201 Google Scholar
[24]	Wang P P, An H H, Fang Z H, Xiong J, Xie Z Y, Wang C, He Z Y, Jia G, Wang R R, Zheng S, Xia L, Feng W, Shi H T, Wang W, Sun J R, Gao Y Q, Fu S Z 2024 Matter Radiat. Extremes 9 015602 Google Scholar
[25]	Lei A, Kang N, Zhao Y, Liu H, An H, Xiong J, Wang R, Xie Z, Tu Y, Xu G, Zhou X, Fang Z, Wang W, Xia L, Feng W, Zhao X, Ji L, Cui Y, Zhou S, Liu Z, Zheng C, Wang L, Gao Y, Huang X, Fu S 2024 Phys. Rev. Lett. 132 035102 Google Scholar
[26]	Rosenberg M, Hernandez J, Butler N, Filkins T, Bahr R, Jungquist R, Bedzyk M, Swadling G, Ross J, Michel P 2021 Rev. Sci Instrum. 92 033511 Google Scholar
[27]	Moody J, Williams E, Glenzer S, Young P, Hawreliak J, Gouveia A, Wark J 2003 Phys. Rev. Lett. 90 245001 Google Scholar
[28]	Froula D, Divol L, Meezan N, Dixit S, Neumayer P, Moody J, Pollock B, Ross J, Suter L, Glenzer S 2007 Phys. Plasmas 14 055705 Google Scholar
[29]	Moody J, MacGowan B, Glenzer S, Kirkwood R, Kruer W, Montgomery D, Schmitt A, Williams E, Stone G 2000 Phys. Plasmas 7 2114 Google Scholar

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