WEKO3
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Therefore, the development of a compact and high-repetition X-ray laser, which can be operated and maintained even in a university laboratory, has been carried out. As major lasing scheme of the X-ray laser, there are two methods, that is, transient collisional excitation scheme and recombination plasma scheme. In the recombination plasma scheme that we focus on, a relatively light element is ionized by laser irradiation onto the metal or gas target and high-temperature and high-density plasma is generated. When the hot, dense plasma is rapidly cooled due to an adiabatic expansion, a non-equilibrium plasma is created, where a three-body recombination process dominate over the other processes. Subsequently, the electron captured into highly-excited states are subjected to collisional deexcitation, resulting in the transition into lower states. 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Lithium-like aluminum ion recombination plasma X-ray laser at 15.5 nm
https://repo.qst.go.jp/records/79352
https://repo.qst.go.jp/records/793523047fa8d-12b6-490a-9aeb-c3fe177bb530
Item type | 会議発表用資料 / Presentation(1) | |||||
---|---|---|---|---|---|---|
公開日 | 2020-03-12 | |||||
タイトル | ||||||
タイトル | Lithium-like aluminum ion recombination plasma X-ray laser at 15.5 nm | |||||
言語 | ||||||
言語 | eng | |||||
資源タイプ | ||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_c94f | |||||
資源タイプ | conference object | |||||
アクセス権 | ||||||
アクセス権 | metadata only access | |||||
アクセス権URI | http://purl.org/coar/access_right/c_14cb | |||||
著者 |
Wang, J.
× Wang, J.× Murakami, K.× R. Shinmori× Kishimoto, Maki× Namba, S.× Kishimoto, Maki |
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抄録 | ||||||
内容記述タイプ | Abstract | |||||
内容記述 | X-ray laser is applied to many scientific and engineering fields such as X-ray microscope, X-ray photoelectron spectroscopy, X-ray lithography, and X-ray holography. Because the plasma-excited X-ray laser is driven by the stimulated emission phenomenon of multiply-charged ions in laser generated plasmas, a driver laser system with an extremely high output energy was necessary. Therefore, the development of a compact and high-repetition X-ray laser, which can be operated and maintained even in a university laboratory, has been carried out. As major lasing scheme of the X-ray laser, there are two methods, that is, transient collisional excitation scheme and recombination plasma scheme. In the recombination plasma scheme that we focus on, a relatively light element is ionized by laser irradiation onto the metal or gas target and high-temperature and high-density plasma is generated. When the hot, dense plasma is rapidly cooled due to an adiabatic expansion, a non-equilibrium plasma is created, where a three-body recombination process dominate over the other processes. Subsequently, the electron captured into highly-excited states are subjected to collisional deexcitation, resulting in the transition into lower states. Consequently, a population inversion between lower levels is generated. The groups of RIKEN and Toyoda Institute of Technology have adopted the recombination plasma scheme and observed the soft X-ray amplification (Li-like Al 3d-4f, 15.5nm) in a high-density Al plasma generated by 16 pulse trains of Nd:YAG laser system. In this study, the similar recombination plasma scheme was employed and lasing experiments were conducted for optimization of laser oscillation on Li-like Al soft X-ray laser. The pumping laser system was a compact Nd:YAG laser (pulse width: 10 ps or 100 ps, pulse interval: 200 ps, total output energy: 2 J for 10 ps laser, 3 J for 100-ps laser, 16 pulse trains), line focusing onto the Al target by a prism array. The laser intensity was 3×10^(11)-1×10^(12) W/cm^2 (focusing size: 0.05 mm×11 mm). Soft X-rays from the laser plasma was measured by a grazing incident spectrometer with a flat field grating. In the experiments,the gain coefficient estimated by the 100-ps laser pulse trains (lasing transition: Li-like 3d-4f 15.5 nm). The gain coefficients obtained are g=8.6 cm-1 and 5.5 cm-1, which is much higher than the value obtained by the previous experiment (g~3.2). Also, we measured the gain coefficient for 10-ps laser pulse train. The optimal laser pulse duration will be discussed in detail. |
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会議概要(会議名, 開催地, 会期, 主催者等) | ||||||
内容記述タイプ | Other | |||||
内容記述 | 3rd Asia-Pacific Conference on Plasma Physics | |||||
発表年月日 | ||||||
日付 | 2019-11-06 | |||||
日付タイプ | Issued |