Author Affiliations
Abstract
1 Key Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
2 Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
Frequency modulation (FM)-to-amplitude modulation (AM) conversion is an important factor that affects the time–power curve of inertial confinement fusion (ICF) high-power laser facilities. This conversion can impact uniform compression and increase the risk of damage to optics. However, the dispersive grating used in the smoothing by spectral dispersion technology will introduce a temporal delay and can spatially smooth the target. The combined effect of the dispersive grating and the focusing lens is equivalent to a Gaussian low-pass filter, which is equivalent to 8 GHz bandwidth and can reduce the intensity modulation on the target to below 5% with 0.3 nm @ 3 GHz + 20 GHz spectrum phase modulation. The results play an important role in the testing and evaluating of the FM-to-AM on the final optics and the target, which is beneficial for comprehensively evaluating the load capacity of the facility and isentropic compression experiment for ICF.
dispersion grating frequency modulation-to-amplitude modulation conversion high-power laser facility inertial confinement fusion phase modulation 
High Power Laser Science and Engineering
2024, 12(1): 010000e9
华翔 1,2,3焦兆阳 1,2,*朱健强 1,2,**
作者单位
摘要
1 中国科学院上海光学精密机械研究所高功率激光物理重点实验室,上海 201800
2 中国科学院中国工程物理研究院高功率激光物理联合实验室,上海 201800
3 中国科学院大学,北京 100049
依靠算法提高光学测量精度的方法和应用越来越广泛,由于刀口法在光学非球面检测中的应用有其独特性,本文提出了在非焦点处采样,对应CCD像面上辅以虚拟光阑调制的刀口法环带,实现定量检测。以检测一个凹球面为例,将其与干涉仪标准方法的检测结果进行对比,其中主要环带位置偏差不超过1%,峰谷(PV)值和均方根(RMS)值误差均在7%左右,可以实现至少λ/15左右的检测灵敏度。该研究为光学车间检测提供了一种定量化检测的新思路,优化了光学加工与检测的效率,为自动化刀口仪的研制奠定了基础。
光学检测 刀口仪 自动化 光学仪器 
光学学报
2023, 43(21): 2112005
刘文凤 1,2孙明营 1,*石逸群 1,2郭亚晶 1[ ... ]朱健强 1,**
作者单位
摘要
1 中国科学院上海光学精密机械研究所高功率激光物理重点实验室,上海 201800
2 中国科学院大学,北京 100049
基于亚纳秒间隔的皮秒激光双脉冲,研究了双脉冲时域整形对K9玻璃表面烧蚀特性的调控规律。当子脉冲间隔为667 ps时,不同形状双脉冲下玻璃表面的烧蚀形貌随激光通量增加的变化规律明显不同,而泵浦通量起着决定性作用。当泵浦通量低于阈值时,双脉冲烧蚀特性基本与单脉冲相似;当泵浦通量在阈值附近时,泵浦脉冲对玻璃表面的微纳米尺度的烧蚀会显著增强探测脉冲的烧蚀效应。当泵浦通量高于1.3倍阈值时,泵浦脉冲在玻璃与空气界面附近产生冲击波,探测脉冲被冲击波的高密度前沿界面反射和干涉,在中心烧蚀区域周围产生了圆环状烧蚀形貌,且圆环分布与探测通量密切相关。双脉冲烧蚀的内径尺寸与泵浦通量相关,而外径尺寸与双脉冲的形状、通量均相关。对比研究了子脉冲间隔为333 ps和667 ps时的等通量双脉冲烧蚀形貌,结果发现:低通量下较小的脉冲间隔可以增强烧蚀效应;高于烧蚀阈值的泵浦脉冲会影响探测脉冲的能量沉积;两种脉冲间隔下环状形貌的不同反映了泵浦脉冲产生的冲击波的传输特性不同。最后基于实验结果讨论了双脉冲序列时域整形进行表面烧蚀调控的物理机制。
激光技术 激光烧蚀 皮秒激光 双脉冲 时域整形 
中国激光
2023, 50(12): 1202201
作者单位
摘要
中国科学院上海光学精密机械研究所高功率激光物理联合实验室,上海 201800
高功率激光装置是一个复杂的有源巨型光学工程,其性能指标要求逼近科学技术与物理极限。驱动器研制有物理设计、工程光学和结构工程设计三大过程,工程光学在其中起着重要作用。高功率激光装置工程光学设计需遵循其特有的设计原则和要点,以保证装置的高性能。根据驱动器设计指标和设计特点,从总体光学设计、光束质量控制以及光束打靶精度控制方面,综述了高功率激光装置工程光学设计中的关键科学技术问题以及相应解决方法,为未来高功率激光驱动器的发展提供必要的工程设计参考。
光学设计 惯性约束聚变 神光装置 工程光学 激光光学 
光学学报
2023, 43(8): 0822005
华翔 1,2,3焦兆阳 1,2朱健强 1,2,*
作者单位
摘要
1 中国科学院上海光学精密机械研究所高功率激光物理重点实验室,上海 201800
2 中国科学院中国工程物理研究院高功率激光物理联合实验室,上海 201800
3 中国科学院大学,北京 100049
为了解决自动化刀口仪面临的如何搜索并收敛到特征点的核心问题,提出一种基于刀口仪轴向移动的非球面检测技术,实现了在搜索过程中提取环带误差信息,一方面在搜索过程中动态获得波前特性,另一方面可以加速收敛找到特征点。利用所提方法对不同参数的镜面环带误差进行检测,所得带差位置与干涉仪检测结果的相对误差小于3.3%,验证了所提方法的有效性。所提方法为刀口仪的自动化测量提供了一个便捷的解决方案,为进一步提高非球面加工效率提供了技术支撑。
测量 刀口仪 自动化 光学检测 光学仪器 
光学学报
2022, 42(23): 2312003
Author Affiliations
Abstract
1 National Laboratory on High Power Laser and Physics, Shanghai 201800, China
2 Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
3 Shanghai Institute of Laser Plasma, Chinese Academy of Engineering and Physics, Shanghai 201800, China
In this paper, we review the status of the multifunctional experimental platform at the National Laboratory of High Power Laser and Physics (NLHPLP). The platform, including the SG-II laser facility, SG-II 9th beam, SG-II upgrade (SG-II UP) facility, and SG-II 5 PW facility, is operational and available for interested scientists studying inertial confinement fusion (ICF) and a broad range of high-energy-density physics. These facilities can provide important experimental capabilities by combining different pulse widths of nanosecond, picosecond, and femtosecond scales. In addition, the SG-II UP facility, consisting of a single petawatt system and an eight-beam nanosecond system, is introduced including several laser technologies that have been developed to ensure the performance of the facility. Recent developments of the SG-II 5 PW facility are also presented.
high-power laser facility inertial confinement fusion solid-state amplifier 
High Power Laser Science and Engineering
2018, 6(4): 04000e55
Author Affiliations
Abstract
1 National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
2 Shanghai Institute of Laser Plasma, Shanghai 201800, China
In high power laser facility for inertial confinement fusion research, final optics assembly (FOA) plays a critical role in the frequency conversion, beam focusing, color separation, beam sampling and debris shielding. The design and performance of FOA in SG-II Upgrade laser facility are mainly introduced here. Due to the limited space and short focal length, a coaxial aspheric wedged focus lens is designed and applied in the FOA configuration. Then the ghost image analysis, the focus characteristic analysis, the B integral control design and the optomechanical design are carried out in the FOA design phase. In order to ensure the FOA performance, two key technologies are developed including measurement and adjustment technique of the wedged focus lens and the stray light management technique based on ground glass. Experimental results show that the design specifications including laser fluence, frequency conversion efficiency and perforation efficiency of the focus spot have been achieved, which meet the requirements of physical experiments well.
final optics assembly high power laser facility inertial confinement fusion. 
High Power Laser Science and Engineering
2018, 6(2): 02000e14
Lei Ren 1,2,†Ping Shao 1,2Dongfeng Zhao 1,2Yang Zhou 1,2[ ... ]Zunqi Lin 1,2
Author Affiliations
Abstract
1 National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
2 Key Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
3 Shanghai Institute of Laser Plasma, China Academy of Engineering Physics, Shanghai 201800, China
The Shen-Guang II Upgrade (SG-II-U) laser facility consists of eight high-power nanosecond laser beams and one short-pulse picosecond petawatt laser. It is designed for the study of inertial confinement fusion (ICF), especially for conducting fast ignition (FI) research in China and other basic science experiments. To perform FI successfully with hohlraum targets containing a golden cone, the long-pulse beam and cylindrical hohlraum as well as the short-pulse beam and cone target alignment must satisfy tight specifications (30 and $20~\unicode[STIX]{x03BC}\text{m}$ rms for each case). To explore new ICF ignition targets with six laser entrance holes (LEHs), a rotation sensor was adapted to meet the requirements of a three-dimensional target and correct beam alignment. In this paper, the strategy for aligning the nanosecond beam based on target alignment sensor (TAS) is introduced and improved to meet requirements of the picosecond lasers and the new six LEHs hohlraum targets in the SG-II-U facility. The expected performance of the alignment system is presented, and the alignment error is also discussed.
laser drivers petawatt lasers spherical hohlraum target alignment target area 
High Power Laser Science and Engineering
2018, 6(1): 01000e10
Author Affiliations
Abstract
National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Science, No. 390, Qinghe Road,Jiading District, Shanghai 201800, China
A model to calculate the optical field distribution of quadruplet beams on a hohlraum target wall is pre-sented. This model combines geometrical ray tracing, coordinate transformation, and Fresnel diffractionintegral to capture the quadruplet beams propagating in four different directions and the typically non-planar geometry of the hohlraum wall. The results demonstrate that the optical field distribution arisesmainly from individual beam diffraction, and the interference with other beams in the quadruplet hardlydevotes to the distribution. A movie is also produced to interpret the spatio and temporal evolution ofthe optical field on a cylindrical hohlraum wall.
Optical field distribution Hohlraum target Quadruplet beams ICF 
Collection Of theses on high power laser and plasma physics
2016, 14(1): 3629–3632
Author Affiliations
Abstract
Chinese Academy of Sciences, Shanghai Institute of Optics and Fine Mechanics, National Laboratory on High Power Laser and Physics, No. 390, Qinghe Road, Jiading District, Shanghai 201800, China
The high fluence performance of high-power laser systems is set by optical damage, especially in the final optics assembly (FOA). The flaws on the frequency converter surface can cause optical intensity intensification and, therefore, damage the downstream optical elements, such as the beam sampling grating (BSG), which is an important component in the FOA. Mitigation of BSG damage caused by flaws is discussed. Physical models are established to simulate the optical field enhancement on BSG modulated by the upstream flaw, considering both the linear and nonlinear propagation effects. Numerical calculations suggest that it is important to place the BSG in a properly selected position to mitigate the laser-induced damage. Furthermore, strict controls of flaw size, modulation depth, distance between frequency converter and focusing lens, and the thickness of the focusing lens are also significant to mitigate the BSG damage. The results obtained could also give some suggestions for damage mitigation of optical components and the layout design of the final optics assembly.
damage mitigation flaw final optics assembly high-power laser hot image 
Collection Of theses on high power laser and plasma physics
2016, 14(1): 011021

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