吴宸 1,2张志远 2徐以会 3宋丽 4[ ... ]刘志 1,3
作者单位
摘要
1 上海科技大学物质科学与技术学院,上海 201210
2 中国科学院上海应用物理研究所,上海 201800
3 上海科技大学大科学中心,上海 201210
4 中国科学院上海高等研究院,上海 201210
为解决硬X射线自由电子激光装置难以提供皮秒至纳秒区间时间分辨的问题,提出了面向目前在建的上海硬X射线自由电子激光装置分束延迟的系统设计。采用基于晶体衍射的延迟方法设计分束延迟光学系统,计算了延迟时间范围,模拟了系统光通量,搭建了一台样机并进行了光路对准实验。该设计采用空间分光方式,将入射脉冲分为两个部分,并通过路程差在二者之间引入时间延迟,具体的原理样机设计适用于光子能量在7~11 keV范围,最多能实现-15.4~503.3 ps的时间延迟。使用Shadow模拟了样机设计的光通量,两个分支光通量分别为33.54%和33.64%,符合1∶1的设计目标。使用绿光激光进行了样机的光路对准实验,证明该样机能使空间分光后的两束光重新复合,为后续X射线验证实验提供基础。该设计具有空间尺寸小、延迟范围大、入射能量和延迟时间连续可调的优点,为上海硬X射线自由电子激光装置的分束延迟系统研制提供参考。
光学设计与制造 分束器 X射线光学 自由电子激光 超快光学 时间延迟 
激光与光电子学进展
2023, 60(1): 0122002
Author Affiliations
Abstract
Shanghai Advanced Research Institute, Chinese Academy of Sciences, Shanghai201210, China
Laser–plasma accelerators (LPAs) have great potential to realize a compact X-ray free-electron laser (FEL), which is limited by the beam properties currently. Two-color high-intensity X-ray FEL provides a powerful tool for probing ultrafast dynamic systems. In this paper, we present a simple and feasible method to generate a two-color X-ray FEL pulse based on an LPA beam. In this scheme, time-dependent mismatch along the bunch is generated and manipulated by the designed lattice system, enabling FEL lasing at different wavelength within two undulator sections. The time separation between the two pulses can be precisely adjusted by varying the time-delay chicane. Numerical simulations show that two-color soft X-ray FELs with gigawatt-level peak power and femtosecond duration can be generated, which confirm the validity and feasibility of the scheme.
free-electron lasers laser–plasma accelerator two-color X-ray 
High Power Laser Science and Engineering
2022, 10(1): 010000e1
Author Affiliations
Abstract
1 SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
2 BELLA Center, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
3 Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany
4 INFN-LNF, 00044 Frascati, Italy
5 LOA, ENSTA Paris, CNRS, Ecole Polytechnique, Institut Polytechnique de Paris, 91762 Palaiseau, France
6 Synchrotron SOLEIL, L’Orme des Merisiers, Saint-Aubin, 91192 Gif-sur-Yvette, France
7 Scottish Centre for the Application of Plasma-Based Accelerators SCAPA, Department of Physics, University of Strathclyde, Scottish Universities Physics Alliance SUPA, Glasgow G1 1XQ, UK
8 Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
9 Department of Physics, University of Strathclyde, Scottish Universities Physics Alliance SUPA, Glasgow G1 1XQ, UK
10 Cockcroft Institute, Warrington WA4 4AD, UK
Owing to their ultra-high accelerating gradients, combined with injection inside micrometer-scale accelerating wakefield buckets, plasma-based accelerators hold great potential to drive a new generation of free-electron lasers (FELs). Indeed, the first demonstration of plasma-driven FEL gain was reported recently, representing a major milestone for the field. Several groups around the world are pursuing these novel light sources, with methodology varying in the use of wakefield driver (laser-driven or beam-driven), plasma structure, phase-space manipulation, beamline design, and undulator technology, among others. This paper presents our best attempt to provide a comprehensive overview of the global community efforts towards plasma-based FEL research and development.
plasma accelerators free electron lasers novel light sources 
High Power Laser Science and Engineering
2021, 9(4): 01000e57
辛明 *
作者单位
摘要
天津大学电气自动化与信息工程学院, 天津 300072
精密定时已成为很多大型先进科学装置的必备技术,而定时精度是这些大型仪器实现其最终目标的关键因素。本文回顾了近年来定时技术的进展,包括不同类型的信号源(激光、微波和X射线脉冲)的定时测量方法,以及基于自由空间链路和光纤的大型定时同步系统。最后简单讨论了目前定时系统的主要限制因素及未来可能的研究方向。
激光光学 定时表征 定时同步 锁模激光器 自由电子激光器 
中国激光
2020, 47(5): 0500007
作者单位
摘要
聊城大学物理科学与信息工程学院山东省光通信科学与技术重点实验室, 山东 聊城 252059
提出了一种基于T形光栅的新型史密斯-珀塞尔自由电子激光器。并利用理论分析和粒子(Particle-in-Cell,PIC)模拟的方法研究了光栅形状对史密斯-珀塞尔自由电子激光器输出特性的影响。理论分析发现,基于T形光栅的史密斯-珀塞尔自由电子激光器的注-波互作用较强,电子束的群聚特性较强,相应地有较强的注-波转换效率,进而有较高的输出功率。PIC模拟发现,基于T形光栅的史密斯-珀塞尔自由电子激光器能够提高辐射功率。在电子束能量E=50 keV、电子束电流i=10 A、光栅周期D=0.3 mm的情况下:基于T形光栅的史密斯-珀塞尔自由电子激光器可以得到0.753949 THz、峰值输出功率约为2 kW的连续太赫兹辐射;而基于矩形光栅的史密斯-珀塞尔自由电子激光器只能得到0.723397 THz、峰值输出功率约为0.3 kW的连续太赫兹辐射。
激光器 史密斯-珀塞尔自由电子激光器 T形光栅 矩形光栅 
光学学报
2020, 40(10): 1014001
Author Affiliations
Abstract
1 State Key Laboratory of High Field Laser Physics , Shanghai Institute of Optics and Fine Mechanics , Chinese Academy of Sciences , Shanghai 201800 , China
2 University of Chinese Academy of Sciences , Beijing 100049 , China
3 Collaborative Innovation Center of IFSA , Shanghai Jiao Tong University , Shanghai 200240 , China
4 School of Physical Science and Technology , ShanghaiTech University, Shanghai 200031 , China
In this study, we investigate a new simple scheme using a planar undulator (PU) together with a properly dispersed electron beam ( beam) with a large energy spread ( ) to enhance the free-electron laser (FEL) gain. For a dispersed beam in a PU, the resonant condition is satisfied for the center electrons, while the frequency detuning increases for the off-center electrons, inhibiting the growth of the radiation. The PU can act as a filter for selecting the electrons near the beam center to achieve the radiation. Although only the center electrons contribute, the radiation can be enhanced significantly owing to the high-peak current of the beam. Theoretical analysis and simulation results indicate that this method can be used for the improvement of the radiation performance, which has great significance for short-wavelength FEL applications.
free-electron lasers X-rays soft X-rays extreme ultraviolet 
High Power Laser Science and Engineering
2018, 6(4): 04000e64
Author Affiliations
Abstract
1 Pohang Accelerator Laboratory, Pohang, Gyeongbuk 790-834, South Korea
2 European XFEL, Notkestrasse 85, 22607 Hamburg, Germany
For the success of PAL-XFEL, two critical systems, namely a low emittance injector and a variable gap out-vacuum undulator, are under development. In order to realize the target emittance of the PAL-XFEL injector we carried out an optimization study of various parameters, such as the laser beam transverse profile, the laser pulse length, the laser phase, and the gun energy. The transverse emittance measured at the Injector Test Facility (ITF) is εx=0.48±0.01 mm mrad. An undulator prototype based on the EU-XFEL design and modified for PAL-XFEL was built and tested. A local-K pole tuning procedure was developed and tested. A significant reduction (90%) of the local-K fluctuation was observed. The requirement of undulator field reproducibility better than 2 ×104 and the undulator gap setting accuracy below 1 μm were achieved for the prototype. The optical phase jitter after the pole height tuning at the tuning gap was calculated to be 2:6_ rms, which satisfies the requirement of 5.0_.
emittance emittance free-electron lasers (FELs) free-electron lasers (FELs) photocathode RF-gun photocathode RF-gun undulator undulator 
High Power Laser Science and Engineering
2015, 3(3): 03000001
Author Affiliations
Abstract
European XFEL GmbH, Albert-Einstein-Ring 18, 22761 Hamburg, Germany
The status of the European X-ray Free-Electron Laser (European XFEL), under construction near Hamburg, Germany, is described. The start of operations of the LCLS at SLAC and of SACLA in Japan has already produced impressive scientific results. The European XFEL facility is powered by a 17.5 GeV superconducting linear accelerator that, compared to these two operating facilities, will generate two orders of magnitude more pulses per second, up to 27 000. It can therefore support modes of operation switching the beam up to 30 times per second among three different experiments, providing each of them with thousands of pulses per second. The scientific possibilities opened up by these capabilities are briefly described, together with the current instrumental developments (in optics, detectors, lasers, etc.) that are necessary to implement this program.
femtosecond lasers and applications femtosecond lasers and applications free-electron lasers and applications free-electron lasers and applications repetition frequency technology repetition frequency technology 
High Power Laser Science and Engineering
2015, 3(3): 03000001
陈世浩 1,2,*陈紫微 3,4,5
作者单位
摘要
1 云南大学岳虹高等研究院, 云南昆明650091
2 东北师范大学理论物理研究所, 吉林长春130024
3 中国科学院电磁辐射与探测技术重点实验室, 北京100190
4 中国科学院大学, 北京100049
5 麻省理工学院, 美国
提出了波长为λi的入射激光与速度为v0、通过波长为λw周期磁场的电子束背散射产生波长λf激光的方案。只要v0足够大,就有λf远小于λi 。扭摆磁铁覆盖有缝隙的超导片后,λw虽不变,但有效背散射区纵向长度s能显著减小。足够强的入射激光也能使s显著减小。与电子束平行的激光谐振腔能产生强度足够大的入射激光。这样,波长λf激光就能实现。即使出射激光的光子数少于入射激光光子数,出射激光的功率仍可以大于入射激光的功率。
激光器 γ-激光 光子-电子背散射 相干条件 自由电子激光 
激光与光电子学进展
2014, 51(9): 091403
张辉 1,2,*张鹏飞 3李一丁 1,2
作者单位
摘要
1 中国科学技术大学 国家同步辐射实验室, 合肥 230029
2 中国科学技术大学 核科学技术学院, 合肥 230029
3 中国科学技术大学 近代物理系, 中国科学院基础等离子体物理重点实验室, 合肥 230026
考虑电子束横向发射度和电子β振荡, 将2005年国际上提出的单通过高增益自由电子激光饱和状态分析的统计物理方法发展到三维情形。首先建立一种描述电子三维运动的归一化简化模型, 推导了一维光场下包含电子横向运动的Vlasov方程。在螺旋型波荡器情形下通过引入横向运动守恒量发展了三维统计物理分析方法, 并编写了相应计算程序, 计算自由电子激光达到饱和时系统的光强增益、聚束因子。作为对比验证, 编写包含N个电子自由电子激光系统的三维直接数值模拟程序, 结果表明数值模拟和统计计算结果相一致。对比文献中一维模拟和一维统计理论计算结果, 所得结果反映了电子束横向发射度以及电子在波荡器中的横向β振荡对饱和点参数的影响。
自由电子激光 统计物理理论 饱和态 数值模拟 横向振荡 相对修正 free electron lasers statistical mechanics methods saturation state numerical simulation transverse oscillation relative correction 
强激光与粒子束
2014, 26(2): 025103

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