Transmission Degradation of Femtosecond Laser Pulses in Opened Cone Targets
Irradiated by femtosecond laser pulses with different energies, opened cone targets behave very differently in the transmission of incident laser pulses. The targets, each with an opening angle of 71° and an opening of 5 μm, are fabricated using standard semiconductor technology. When the incident l...
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| Published in | Plasma science & technology Vol. 14; no. 1; pp. 24 - 27 |
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| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
2012
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| Subjects | |
| Online Access | Get full text |
| ISSN | 1009-0630 |
| DOI | 10.1088/1009-0630/14/1/06 |
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| Abstract | Irradiated by femtosecond laser pulses with different energies, opened cone targets behave very differently in the transmission of incident laser pulses. The targets, each with an opening angle of 71° and an opening of 5 μm, are fabricated using standard semiconductor technology. When the incident laser energy is low and no pre-plasma is generated on the side walls of the cones, the cone target acts like an optical device to reflect the laser pulse, and 15% of the laser energy can be transmitted through the cones. In contrast, when the incident laser energy is high enough to generate pre-plasmas by the pre-pulse of the main pulse that fills the inner cone, the cone with the plasmas will block the transmission of the laser, which leads to a decrease in laser transmission compared with the low-energy case with no plasma. Simulation results using optical software in the low-energy case, and using the particle-in-cell code in the high-energy case, are primarily in agreement with the experimental results. |
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| AbstractList | Irradiated by femtosecond laser pulses with different energies, opened cone targets behave very differently in the transmission of incident laser pulses. The targets, each with an opening angle of 71° and an opening of 5 μm, are fabricated using standard semiconductor technology. When the incident laser energy is low and no pre-plasma is generated on the side walls of the cones, the cone target acts like an optical device to reflect the laser pulse, and 15% of the laser energy can be transmitted through the cones. In contrast, when the incident laser energy is high enough to generate pre-plasmas by the pre-pulse of the main pulse that fills the inner cone, the cone with the plasmas will block the transmission of the laser, which leads to a decrease in laser transmission compared with the low-energy case with no plasma. Simulation results using optical software in the low-energy case, and using the particle-in-cell code in the high-energy case, are primarily in agreement with the experimental results. |
| Author | 刘峰 林晓宣 刘必成 丁文君 杜飞 李玉同 马景龙 刘晓龙 盛政明 陈黎明 鲁欣 董全力 王伟民 王兆华 魏志义 陈佳洱 张杰 |
| AuthorAffiliation | Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China Key Laboratory for Laser Plasmas (MoE) and Department of Physics, Shanghai Jiao Tong University, Shanghai 200240, China State Key Laboratory of Nuclear Physics and Technology, Institute of Heavy Ion Physics, Peking University, Beijing 100871, China |
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| Cites_doi | 10.1103/PhysRevLett.96.165003 10.1063/1.2903054 10.1088/0029-5515/49/10/104024 10.1364/OE.16.000081 10.1063/1.3121220 10.1063/1.2890124 10.1063/1.870664 10.1364/AO.46.002498 10.1038/35090525 10.1038/418933a 10.1016/S0924-4247(97)01658-0 10.1063/1.1735734 10.1103/PhysRevLett.104.055002 |
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| Notes | Irradiated by femtosecond laser pulses with different energies, opened cone targets behave very differently in the transmission of incident laser pulses. The targets, each with an opening angle of 71° and an opening of 5 μm, are fabricated using standard semiconductor technology. When the incident laser energy is low and no pre-plasma is generated on the side walls of the cones, the cone target acts like an optical device to reflect the laser pulse, and 15% of the laser energy can be transmitted through the cones. In contrast, when the incident laser energy is high enough to generate pre-plasmas by the pre-pulse of the main pulse that fills the inner cone, the cone with the plasmas will block the transmission of the laser, which leads to a decrease in laser transmission compared with the low-energy case with no plasma. Simulation results using optical software in the low-energy case, and using the particle-in-cell code in the high-energy case, are primarily in agreement with the experimental results. LIU Feng , LIN Xiaoxuan, LIU Bicheng , DING Wenjun , DU Fei , LI Yutong , MA Jinglong, LIU Xiaolong, SHENG Zhengming , CHEN Liming , LU Xin , DONG Quanli , WANG Weimin , WANG Zhaohua, WEI Zhiyi , CHEN Jiaer, ZHANG Jie (1.Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China 2Key Laboratory for Laser Plasmas (MoE) and Department of Physics, Shanghai Jiao Tong University, Shanghai 200240, China 3State Key Laboratory of Nuclear Physics and Technology, Institute of Heavy Ion Physics, Peking University, Beijing 100871, China) 34-1187/TL femtosecond laser pulse, cone target, transmission ratio |
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| References | 11 Azechi Hiroshi (3) 2009; 49 12 13 1 2 4 5 6 7 8 9 10 |
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| Snippet | Irradiated by femtosecond laser pulses with different energies, opened cone targets behave very differently in the transmission of incident laser pulses. The... |
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| SubjectTerms | 光学装置 半导体技术 开业 激光传输 激光能量 等离子体产生 降解 飞秒激光脉冲 |
| Title | Transmission Degradation of Femtosecond Laser Pulses in Opened Cone Targets |
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