Wei-Man Jiang1、2, Yu-Tong Li1、2、7、*, Zhe Zhang1、*, Bao-Jun Zhu1、2, Yi-Hang Zhang1、2, Da-Wei Yuan3, Hui-Gang Wei3, Gui-Yun Liang3, Bo Han4, Chang Liu4, Xiao-Xia Yuan4, Neng Hua5, Bao-Qiang Zhu5, Jian-Qiang Zhu5, Zhi-Heng Fang6, Chen Wang6, Xiu-Guang Huang6, and Jie Zhang1、7、8
Author Affiliations
1Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China2School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China3National Astronomical Observatories, Chinese Academy of Science, Beijing 100012, China4Department of Astronomy, Beijing Normal University, Beijing 100875, China5Shanghai Institute of Optical and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China6Shanghai Institute of Laser Plasma, China Academy of Engineering Physics, Shanghai 201800, China7Songshan Lake Materials Laboratory, Dongguan 523808, China8Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University, Shanghai 200240, Chinashow less
DOI: 10.7498/aps.68.20190501
Cite this Article
Wei-Man Jiang, Yu-Tong Li, Zhe Zhang, Bao-Jun Zhu, Yi-Hang Zhang, Da-Wei Yuan, Hui-Gang Wei, Gui-Yun Liang, Bo Han, Chang Liu, Xiao-Xia Yuan, Neng Hua, Bao-Qiang Zhu, Jian-Qiang Zhu, Zhi-Heng Fang, Chen Wang, Xiu-Guang Huang, Jie Zhang. Effect of laser intensity on microwave radiation generated in nanosecond laser-plasma interactions[J]. Acta Physica Sinica, 2019, 68(12): 125201-1
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Fig. 1. Experimental setup.实验布局图
Fig. 2. Peak E-field magnitude versus laser intensity in the four different directions.
不同激光强度下, 四个方向上对应的电场峰幅值
Fig. 3. Electric field waveforms detected by the monopole antenna-3 at laser intensities of (a) 5.7 × 1014, (b) 7.4 × 1014, (c) 1.5 × 1015, (d) 2.0 × 1015, (e) 2.9 × 1015, and (f) 6.2 × 1015 W/cm2.
入射激光强度分别为(a) 5.7 × 1014, (b) 7.4 × 1014, (c) 1.5 × 1015, (d) 2.0 × 1015, (e) 2.9 × 1015, (f) 6.2 × 1015 W/cm2时, 靶前靠近法线方向上的电场时间波形
Fig. 4. Frequency spectra of the electric fields detected by the monopole antenna-3 at laser intensities of (a) 5.7 × 1014, (b) 7.4 × 1014, (c) 1.5 × 1015, (d) 2.0 × 1015, (e) 2.9 × 1015, and (f) 6.2 × 1015 W/cm2.
入射激光强度分别为(a) 5.7 × 1014, (b) 7.4 × 1014, (c) 1.5 × 1015, (d) 2.0 × 1015, (e) 2.9 × 1015, (f) 6.2 × 1015 W/cm2时, 靶前靠近法线方向上电场的频谱分布
Fig. 5. Electric field waveforms and their corresponding frequency spectra detected by the four monopole antennas. (a) and (e) correspond to the monopole antenna-1, (b) and (f) correspond to the monopole antenna-2, (c) and (g) correspond to the monopole antenna-3, (d) and (h) correspond to the monopole antenna-4. The laser intensity is 1.5 × 1015 W/cm2.
入射激光强度为1.5 × 1015 W/cm2时, 不同方向测量的电场波形及其频谱分布 (a)和(e)对应单极天线-1; (b)和(f)对应单极天线-2; (c)和(g)对应单极天线-3; (d)和(h)对应单极天线-4
Fig. 6. Electric field waveforms and their corresponding frequency spectra detected by the four monopole antennas. (a) and (e) correspond to the monopole antenna-1, (b) and (f) correspond to the monopole antenna-2, (c) and (g) correspond to the monopole antenna-3, (d) and (h) correspond to the monopole antenna-4. The laser intensity is 6.2 × 1015 W/cm2.
入射激光强度为6.2 × 1015 W/cm2时, 不同方向测量的电场波形及其频谱分布 (a)和(e)对应单极天线-1; (b)和(f)对应单极天线-2; (c)和(g)对应单极天线-3; (d)和(h)对应单极天线-4
Fig. 7. Radiation energy versus laser intensity at different directions: (a) Total radiation energy detected by the antennas; (b) radiation energy at frequencies lower than 0.3 GHz; (c) radiation energy at frequencies upper than 0.3 GHz.不同方向测量的微波辐射能量随激光强度的变化(a)单位立体角内产生的总辐射能; (b)单位立体角内产生的0.3 GHz以下的辐射能; (c)单位立体角内产生的0.3 GHz以上的辐射能