Author Affiliations
Abstract
1 MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai 200092, China
2 Institute of Precision Optical Engineering, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
3 Center for Transformative Science, ShanghaiTech University, Shanghai 201210, China
In this paper, a simple theoretical model combining Monte Carlo simulation with the enthalpy method is provided to simulate the damage resistance of B4C/Si-sub mirror under X-ray free-electron laser irradiation. Two different damage mechanisms are found, dependent on the photon energy. The optimum B4C film thickness is determined by studying the dependence of the damage resistance on the film thickness. Based on the optimized film thickness, the damage thresholds are simulated at photon energy of 0.4–25 keV and a grazing incidence angle of 2 mrad. It is recommended that the energy range around the Si K-edge should be avoided for safety reasons.
B4C film XFEL damage mechanism damage threshold enthalpy method 
Chinese Optics Letters
2023, 21(2): 023401
T. Pikuz 1,2,3,*A. Faenov 2,3N. Ozaki 1,4T. Matsuoka 3[ ... ]R. Kodama 1,3,4,8
Author Affiliations
Abstract
1 Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871, Japan
2 Joint Institute for High Temperatures, Russian Academy of Sciences, Moscow 125412, Russia
3 Open and Transdisciplinary Research Initiatives, Osaka University, Suita, Osaka 565-0871, Japan
4 Photon Pioneers Center, Osaka University, Suita, Osaka 565-0871, Japan
5 LULI - CNRS, Ecole Polytechnique, CEA: Universite Paris-Saclay
6 UPMC Univ Paris 06: Sorbonne Universites - F-91128 Palaiseau cedex, France
7 Helmholtz-Zentrum Dresden-Rossendorf, Dresden 01328, Germany
8 ILE, Osaka University, Suita, Osaka 565-0871, Japan
9 Japan Synchrotron Radiation Research Institute, Sayo-cho, Sayo-gun, Hyogo 679-5198, Japan
10 RIKEN Spring-8 Center, Sayo-cho, Sayo-gun, Hyogo 679-5148, Japan
11 Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University, Moscow 119991, Russia
12 Universite de Bordeaux-CNRS-CEA, CELIA (Center Lasers Intenses et Applications), UMR 5107, F-33405 Talence, France
13 National Research Nuclear University MEPhI, Moscow 115409, Russia
14 LULI- CNRS, Ecole Polytechnique, CEA: Universite Paris-Saclay
15 ELI-NP/IFN-HH, Maqurele-Bucharest 077125 Romania
We present new diagnostics for use in optical laser pump - X-ray Free Electron Laser (XFEL) probe experiments to monitor dimensions, intensity profile and focusability of the XFEL beam and to control initial quality and homogeneity of targets to be driven by optical laser pulse. By developing X-ray imaging, based on the use of an LiF crystal detector, we were able to measure the distribution of energy inside a hard X-ray beam with unprecedented high spatial resolution (~1 mm) and across a field of view larger than some millimetres. This diagnostic can be used in situ, provides a very high dynamic range, has an extremely limited cost, and is relatively easy to be implemented in pumpprobe experiments. The proposed methods were successfully applied in pump-probe experiments at the SPring-8 Angstrom Compact free electron LAser (SACLA) XFEL facility and its potential was demonstrated for current and future High Energy Density Science experiments.
XFEL XFEL Shock waves Shock waves Pump-probe experiments Pump-probe experiments High energy density science High energy density science X-ray spectroscopy X-ray spectroscopy X-ray imaging X-ray imaging 
Matter and Radiation at Extremes
2018, 3(4): 197
Author Affiliations
Abstract
1 RIKEN, SPring-8 Center, Kouto 1-1-1, Sayo, Hyogo 679-5148, Japan
2 Japan Synchrotron Radiation Research Institute, Kouto 1-1-1, Sayo, Hyogo 679-5198, Japan
3 RIKEN Center for Advanced Photonics, Hirosawa 2-1, Wako, Saitama 351-0198, Japan
4 Japan Atomic Energy Agency, Umemidai 8-1-7, Kizugawa, Kyoto 619-0215, Japan
5 The University of Tokyo, Hongo 7-3-1, Bunkyo-ku, Tokyo 113-0033, Japan
A fully coherent free electron laser (FEL) seeded with a higher-order harmonic (HH) pulse from high-order harmonic generation (HHG) is successfully operated for a sufficiently prolonged time in pilot user experiments by using a timing drift feedback. For HHG-seeded FELs, the seeding laser pulses have to be synchronized with electron bunches. Despite seeded FELs being non-chaotic light sources in principle, external laser-seeded FELs are often unstable in practice because of a timing jitter and a drift between the seeding laser pulses and the accelerated electron bunches. Accordingly, we constructed a relative arrival-timing monitor based on non-invasive electro-optic sampling (EOS). The EOS monitor made uninterrupted shot-to-shot monitoring possible even during the seeded FEL operation. The EOS system was then used for arrival-timing feedback with an adjustability of 100 fs for continual operation of the HHG-seeded FEL. Using the EOS-based beam drift controlling system, the HHG-seeded FEL was operated over half a day with an effective hit rate of 20%–30%. The output pulse energy was 20 mJ at the 61.2 nm wavelength. Towards seeded FELs in the water window region, we investigated our upgrade plan to seed high-power FELs with HH photon energy of 30–100 eV and lase at shorter wavelengths of up to 2 nm through high-gain harmonic generation (HGHG) at the energy-upgraded SPring-8 Compact SASE Source (SCSS) accelerator. We studied a benefit as well as the feasibility of the next HHG-seeded FEL machine with single-stage HGHG with tunability of a lasing wavelength.
arrival-timing monitor arrival-timing monitor electro-optic sampling (EOS) electro-optic sampling (EOS) high-gain harmonic generation (HGHG) high-gain harmonic generation (HGHG) high-order harmonic generation (HHG) high-order harmonic generation (HHG) self-amplified spontaneous emission (SASE) self-amplified spontaneous emission (SASE) the soft x-ray water window region the soft x-ray water window region wavelength-tunable seeded FEL wavelength-tunable seeded FEL X-ray free electron laser (XFEL) X-ray free electron laser (XFEL) 
High Power Laser Science and Engineering
2015, 3(2): 02000001
作者单位
摘要
1 中国科学院 高能物理研究所, 北京 100049
2 中国科学院 研究生院, 北京 100049
3 中国科学院 上海应用物理研究所, 上海 201800
分析了X射线自由电子激光装置对飞秒同步定时系统的技术需求。系统中采用光纤来传输定时/相位信息。而光纤的光长度会随温度的慢漂而改变,因此通过对比实验研究了温度慢漂对光纤长度变化的影响。研制了基于现场可编程门阵列(FPGA)的数字化相位和幅度检测器对光纤长度变化进行数据监测。百米光纤在典型昼夜温差下导致的时间延迟约6 ps。结果显示此数字化相位和幅度检测器可以用于飞秒同步定时系统的长度变化监测和稳定控制系统当中。
长度变化 数字化相位和幅度检测器 现场可编程门阵列 X射线自由电子激光 飞秒同步与定时 length variation digital phase/amplitude detector FPGA XFEL femtosecond timing and synchronization 
强激光与粒子束
2012, 24(2): 297

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