作者单位
摘要
1 山西大学 激光光谱研究所 量子光学与光量子器件国家重点实验室, 山西 太原 030006
2 山西大学 极端光学协同创新中心, 山西 太原 030006
3 中石油化工股份有限公司石油化工科学研究院, 北京 100083
4 中国兵器科学研究院, 北京 100089
5 山西新华防化装备研究院有限公司, 山西 太原 030041
6 西安工业大学 光电工程学院, 陕西 西安 710021
7 山西格盟中美清洁能源研发中心有限公司, 山西 太原 030032
为了消除激光诱导击穿光谱技术(laser-induced breakdown spectroscopy,LIBS)中的自吸收效应,提高元素定量分析的精确度,同时满足工业中便捷分析元素的要求,需将自吸收免疫激光诱导击穿光谱技术(self-absorption free laser-induced breakdown spectroscopy,SAF-LIBS)的装置小型化。本文提出了一项新型的高重频声光门控SAF-LIBS定量分析技术,使用高重频激光器产生准连续的等离子体以增强光谱强度,并将声光调制器(acousto-optic modulator,AOM)作为门控开关,从而使微型CCD光谱仪和AOM能够代替传统大型SAF-LIBS装置中的像增强探测器(intensified charge coupled device,ICCD)和中阶梯型光栅光谱仪,实现自吸收免疫的同时缩小了装置的体积,降低了装置的成本。将该系统参数进行优化选择后,对样品中的Al元素进行了定量分析和预测。实验结果表明,等离子体的特性受激光重复频率的影响进而会影响光谱信号的强度。在1 ~ 50 kHz激光重复频率范围内,Al I 394.4 nm和Al I 396.15 nm的双线强度先增强后减弱,确定最佳的激光重复频率为10 kHz。在不同的光纤采集角度下,Al的双线强度比随延迟时间的增加而减小,在45°处信噪比最高,且在一定的积分时间下,最佳光学薄时间tot为426 ns。在激光重复频率为10 kHz、光纤采集角为45°、延迟时间为400 ns的条件下,对Al元素进行定量分析和预测结果表明,Al元素定标曲线的线性度R2为0.982,平均绝对测量误差相对于单一LIBS的0.8%可以降低至0.18%。定量分析结果与传统大型SAF-LIBS装置的测量精度相持平。因此本高重频声光门控SAF-LIBS装置不仅有效地屏蔽了光学厚等离子体中的连续背景辐射和谱线加宽,同时具备小型化、低成本、高可靠性的优点,有助于推动SAF-LIBS技术由实验室走向工业应用。
激光诱导击穿光谱 自吸收免疫 光学薄 高重频激光器 声光门控 laser-induced breakdown and spectroscopy self-absorption free optically thin high repetition rate laser acousto-optic gating 
中国光学
2024, 17(2): 253
Author Affiliations
Abstract
1 Department of Engineering Physics, Air Force Institute of Technology, WPAFB, OH, USA
2 Physics Department, Marietta College, Marietta, OH, USA
3 Department of Physics, The Ohio State University, Columbus, OH, USA
4 Department of Materials Science and Engineering, and Department of Electrical and Computer Science, The Ohio State University, Columbus, OH, USA
5 Intense Energy Solutions, LLC, Plain City, OH, USA
We present detailed characterization of laser-driven fusion and neutron production ( $\sim {10}^5$ /second) using 8 mJ, 40 fs laser pulses on a thin (<1 μm) D ${}_2$ O liquid sheet employing a measurement suite. At relativistic intensity ( $\sim 5\times {10}^{18}$ W/cm ${}^2$ ) and high repetition rate (1 kHz), the system produces deuterium–deuterium (D-D) fusion, allowing for consistent neutron generation. Evidence of D-D fusion neutron production is verified by a measurement suite with three independent detection systems: an EJ-309 organic scintillator with pulse-shape discrimination, a ${}^3\mathrm{He}$ proportional counter and a set of 36 bubble detectors. Time-of-flight analysis of the scintillator data shows the energy of the produced neutrons to be consistent with 2.45 MeV. Particle-in-cell simulations using the WarpX code support significant neutron production from D-D fusion events in the laser–target interaction region. This high-repetition-rate laser-driven neutron source could provide a low-cost, on-demand test bed for radiation hardening and imaging applications.
high-repetition-rate laser-driven fusion laser–plasma interaction liquid target neutron detectors 
High Power Laser Science and Engineering
2024, 12(1): 010000e2
Author Affiliations
Abstract
1 Centre Lasers Intenses et Applications (CELIA), Université de Bordeaux–CNRS–CEA, Talence cedex, France
2 ENEA, Fusion and Technology for Nuclear Safety and Security Department, C.R. Frascati, Frascati, Italy
3 AWE, Aldermaston, Reading, UK
4 Centre for Inertial Fusion Studies, Blackett Laboratory, Imperial College London, London, UK
5 Istituto Nazionale di Ottica, Consiglio Nazionale delle Ricerche (CNR-INO), Pisa, Italy
6 ETSIAE Universidad Politecnica de Madrid, Madrid, Spain
7 GSI-Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
8 Laboratoire pour l’Utilisation des Lasers Intenses (LULI), CNRS–Ecole Polytechnique, Palaiseau cedex, France
9 ALP, Le Barp, France and CEA/DAM Île de France, Bruyères le Châtel, Arpajon cedex, France
10 Instituto Fusión Nuclear “Guillermo Velarde” (IFN-GV), Universidad Politecnica de Madrid, Madrid, Spain
11 Central Laser Facility, STFC Rutherford Appleton Laboratory, Harwell Oxford, Oxfordshire, UK
12 Institute of Plasma Physics and Lasers, University Research and Innovation Centre, Hellenic Mediterranean University, Rethymno, Crete, Greece
13 Department of Electronic Engineering, School of Engineering, Hellenic Mediterranean University, Chania, Crete, Greece
14 Extreme Light Infrastructure ERIC, ELI-Beamlines Facility, Dolní Břežany, Czech Republic
15 Centro de Laseres Pulsados (CLPU), Parque Cientifico, Villamayor, Salamanca, Spain
The recent achievement of fusion ignition with laser-driven technologies at the National Ignition Facility sets a historic accomplishment in fusion energy research. This accomplishment paves the way for using laser inertial fusion as a viable approach for future energy production. Europe has a unique opportunity to empower research in this field internationally, and the scientific community is eager to engage in this journey. We propose establishing a European programme on inertial-fusion energy with the mission to demonstrate laser-driven ignition in the direct-drive scheme and to develop pathway technologies for the commercial fusion reactor. The proposed roadmap is based on four complementary axes: (i) the physics of laser–plasma interaction and burning plasmas; (ii) high-energy high repetition rate laser technology; (iii) fusion reactor technology and materials; and (iv) reinforcement of the laser fusion community by international education and training programmes. We foresee collaboration with universities, research centres and industry and establishing joint activities with the private sector involved in laser fusion. This project aims to stimulate a broad range of high-profile industrial developments in laser, plasma and radiation technologies along with the expected high-level socio-economic impact.
education and training fusion reactor technology high-energy laser high repetition rate laser inertial confinement fusion laser–plasma interaction public–private partnership radiation resistant materials 
High Power Laser Science and Engineering
2023, 11(6): 06000e83
Author Affiliations
Abstract
1 School of Mathematics and Physics, Queen’s University Belfast, Belfast, UK
2 Central Laser Facility, STFC Rutherford Appleton Laboratory, Didcot, UK
3 Gérard Mourou Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI, USA
4 SLAC National Accelerator Laboratory, Menlo Park, CA, USA
5 Department of Electrical and Computer Engineering, University of Alberta, Edmonton, AB, Canada
6 The John Adams Institute for Accelerator Science, Imperial College London, London, UK
7 ELI Beamlines Centre, Institute of Physics, Czech Academy of Sciences, Dolní Břežany, Czech Republic
8 Department of Applied Physics, Stanford University, Stanford, CA, USA
9 Department of Physics, SUPA, University of Strathclyde, Glasgow, UK
10 Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
11 Department of Mechanical Engineering, Stanford University, Stanford, CA, USA
12 Institut für Kernphysik, Technische Universität Darmstadt, Darmstadt, Germany
The interaction of relativistically intense lasers with opaque targets represents a highly non-linear, multi-dimensional parameter space. This limits the utility of sequential 1D scanning of experimental parameters for the optimization of secondary radiation, although to-date this has been the accepted methodology due to low data acquisition rates. High repetition-rate (HRR) lasers augmented by machine learning present a valuable opportunity for efficient source optimization. Here, an automated, HRR-compatible system produced high-fidelity parameter scans, revealing the influence of laser intensity on target pre-heating and proton generation. A closed-loop Bayesian optimization of maximum proton energy, through control of the laser wavefront and target position, produced proton beams with equivalent maximum energy to manually optimized laser pulses but using only 60% of the laser energy. This demonstration of automated optimization of laser-driven proton beams is a crucial step towards deeper physical insight and the construction of future radiation sources.
Bayesian optimization high repetition-rate laser–target interaction laser-driven particle acceleration proton generation 
High Power Laser Science and Engineering
2023, 11(3): 03000e35
Author Affiliations
Abstract
1 John Adams Institute for Accelerator Science, Blackett Laboratory, Imperial College London, London, UK
2 School of Maths and Physics, Queen’s University Belfast, Belfast, UK
3 Central Laser Facility, STFC Rutherford Appleton Laboratory, Didcot, UK
4 SLAC National Accelerator Laboratory, Menlo Park, USA
5 ELI Beamlines Centre, Institute of Physics, CAS, Dolni Brezany, Czech Republic
6 Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
7 Department of Physics, SUPA, University of Strathclyde, Glasgow, UK
8 Department of Mechanical Engineering, Stanford University, Stanford, USA
9 Department of Applied Physics, Stanford University, Stanford, USA
10 Department of Electrical and Computer Engineering, University of Alberta, Edmonton, Canada
11 Institut für Kernphysik, Technische Universität Darmstadt, Darmstadt, Germany
We present the development and characterization of a high-stability, multi-material, multi-thickness tape-drive target for laser-driven acceleration at repetition rates of up to 100 Hz. The tape surface position was measured to be stable on the sub-micrometre scale, compatible with the high-numerical aperture focusing geometries required to achieve relativistic intensity interactions with the pulse energy available in current multi-Hz and near-future higher repetition-rate lasers ( $>$ kHz). Long-term drift was characterized at 100 Hz demonstrating suitability for operation over extended periods. The target was continuously operated at up to 5 Hz in a recent experiment for 70,000 shots without intervention by the experimental team, with the exception of tape replacement, producing the largest data-set of relativistically intense laser–solid foil measurements to date. This tape drive provides robust targetry for the generation and study of high-repetition-rate ion beams using next-generation high-power laser systems, also enabling wider applications of laser-driven proton sources.
high-repetition-rate laser target laser–plasma acceleration proton generation tape-drive target 
High Power Laser Science and Engineering
2023, 11(2): 02000e23
Author Affiliations
Abstract
1 School of Information and Communication Engineering, North University of China, Taiyuan 030051, China
2 Department of Physics, Korea Advanced Institute of Science and Technology, Daejeon 34141, Republic of Korea
3 School of Electronics and Information Engineering, Hebei University of Technology, Tianjin 300401, China
Thermal effects are typically considered as obstacles to high-repetition-rate stimulated Brillouin scattering (SBS) pulse compression. In this paper, a novel method is proposed for improving the SBS output characteristics by exploiting thermal effects on the liquid medium. Using HT270, the SBS output parameters with the medium purification and rotating off-centered lens methods are studied at different repetition rates. The results indicate that these two methods can alleviate thermal effects and improve the energy efficiency, but the rotating method reduces the energy stability because of the aggravated optical breakdown at the kilohertz-level repetition rate. For a 35-mJ pump energy, the energy efficiency at 2 kHz without the rotating method is 30% higher than that at 100 Hz and 70% higher than that at 500 Hz. The enhancement of the SBS output characteristics by thermal effects is demonstrated theoretically and experimentally, and 2-kHz high-power SBS pulse compression is achieved with HT270.
high-repetition-rate laser stimulated Brillouin scattering pulse compression thermal effects 
High Power Laser Science and Engineering
2022, 10(4): 04000e24
作者单位
摘要
1 火箭军工程大学,西安 710000
2 中国人民解放军96922部队,辽宁 大连 116000
对高重频激光诱饵重复频率选择进行了研究。首先从高重频激光诱饵干扰原理出发, 通过对其干扰脉冲能量和重复频率的理论分析和数值计算, 得出了高重频诱饵频率运用方案, 最后通过干扰效果实验对方案进行了验证, 研究结果表明: 高重频激光诱饵实施诱偏干扰, 高重频干扰脉冲重复频率必须是指示激光脉冲频率的整数倍; 相比于激光导引头跟踪阶段诱偏干扰, 需要高重频干扰脉冲具有较高重复频率以保证至少有3~4个干扰脉冲进入时间波门, 高重频激光诱饵在激光导引头搜索阶段进行干扰只需要较低的重复频率就能达到理想的诱偏干扰效果。
高重频激光诱饵 能量 重复频率 干扰效果实验 high-repetition-rate laser decoy energy repetition rate jamming effect experiment 
电光与控制
2022, 29(4): 72
作者单位
摘要
1 中国科学院 宁波材料技术与工程研究所,浙江宁波3520
2 宁波大艾激光科技有限公司,浙江宁波31501
为了提高化学气相沉积(Chemical Vapor Deposition,CVD)金刚石的切深,采用新型的声光调制高重复频率激光器,研究了激光功率、焦点位置、激光重复频率、切割线速度以及激光横膜模式对CVD金刚石切缝宽度、切深以及表面粗糙度的影响。研究结果表明:切深和切缝上表面宽随着激光功率的增大而增大;焦点位置随切深的变化下移,可获得最大切深;重复频率的增大伴随着切深的减小和切缝上表面宽的增大;表面粗糙度随着切割线速度的增大先缓慢减小后显著增大;切缝上表面宽随着模式数的增多而增大。综合切深、缝宽和效率,最后在输出基横模下激光功率为12 W,重复频率为6 kHz,切割线速度为1 500 mm/min,焦点位置始终位于切割凹面,获得了效率最快、质量最好的结果,即单向切深最大可达7.2 mm,切面表面的粗糙度为0.804 µm,切缝上表面宽度为350 µm,满足在低切面表面粗糙度下获得CVD金刚石大切深的要求。
激光切割 化学气相沉积金刚石 高频激光 缝宽 切深 表面粗糙度 laser cutting chemical vapor deposition diamond high repetition rate laser width of cutting seam cutting depth surface roughness 
光学 精密工程
2022, 30(1): 89
Songqing Zha 1,2Yujin Chen 1,*Bingxuan Li 1,3Yanfu Lin 1[ ... ]Ge Zhang 1,3,5,**
Author Affiliations
Abstract
1 Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou 350002, China
2 Fuzhou University, Fuzhou 350002, China
3 Fujian Science & Technology Innovation Laboratory for Optoelectronic Information of China, Fuzhou 350108, China
4 Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, China
5 Collaborative Innovation Center for Optoelectronic Semiconductors and Efficient Device, Fuzhou 350108, China
End-pumped by a 976 nm diode laser, a high-repetition-rate Er:Yb:YAl3(BO3)4 microchip laser passively Q-switched by a Co2+:MgAl2O4 crystal is reported. At a quasi-continuous-wave pump power of 20 W, a 1553 nm passively Q-switched laser with the repetition rate of 544 kHz, pulse duration of 8.3 ns, and pulse energy of 3.9 μJ was obtained. To the best of our knowledge, the 544 kHz is the highest reported value for the 1.5 μm passively Q-switched pulse laser. In the continuous-wave pumping experiment, the maximum repetition rate of 144 kHz with the pulse duration of 8.0 ns and pulse energy of 1.7 μJ was obtained at the incident pump power of 6.3 W.
1.5?μm microchip laser passive Q-switching Er:Yb:YAl34 crystal high-repetition-rate laser pulse 
Chinese Optics Letters
2021, 19(7): 071402
作者单位
摘要
海军工程大学兵器工程学院, 湖北 武汉 430033
为了评价高重复频率系统在每个选通切片中的成像质量,为脉冲分配策略的研究提供依据,在Jaffe-McGlamery模型的基础上,建立描述高重复频率系统信号传输过程的理论模型,分析图像退化因素,提出一种高重复频率系统成像质量评价模型。采用重复频率为4 kHz的脉冲激光器,对黑白条纹靶板目标进行成像。实验结果表明,从目标开始成像到出现饱和前的线性区间内,该理论模型的结果与实验结果相吻合,误差不超过10%。
海洋光学 对比度信噪比 高重复频率激光成像系统 成像雷达 
中国激光
2019, 46(7): 0701003

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