Plasma density limits for hole boring by intense laser pulses

被引:39
作者
Iwata, Natsumi [1 ]
Kojima, Sadaoki [1 ,2 ]
Sentoku, Yasuhiko [1 ]
Hata, Masayasu [1 ]
Mima, Kunioki [3 ]
机构
[1] Osaka Univ, Inst Laser Engn, 2-6 Yamadaoka, Suita, Osaka 5650871, Japan
[2] Kyoto Univ, Inst Chem Res, Adv Res Ctr Beam Sci, Uji, Kyoto 6110011, Japan
[3] Grad Sch Creat New Photon Ind, Nishi Ku, 1955-1 Kurematsu, Hamamatsu, Shizuoka 1411201, Japan
关键词
ION-ACCELERATION; FAST IGNITION; GENERATION; FUSION; BEAMS;
D O I
10.1038/s41467-018-02829-5
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
High-power lasers in the relativistic intensity regime with multi-picosecond pulse durations are available in many laboratories around the world. Laser pulses at these intensities reach giga-bar level radiation pressures, which can push the plasma critical surface where laser light is reflected. This process is referred to as the laser hole boring (HB), which is critical for plasma heating, hence essential for laser-based applications. Here we derive the limit density for HB, which is the maximum plasma density the laser can reach, as a function of laser intensity. The time scale for when the laser pulse reaches the limit density is also derived. These theories are confirmed by a series of particle-in-cell simulations. After reaching the limit density, the plasma starts to blowout back toward the laser, and is accompanied by copious superthermal electrons; therefore, the electron energy can be determined by varying the laser pulse length.
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页数:7
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