Author Affiliations
Abstract
1 Intense Laser Irradiation Laboratory (ILIL), Istituto Nazionale di Ottica – Consiglio Nazionale delle Ricerche (INO-CNR), Sede Secondaria di Pisa, Via Moruzzi, 1, 56124 Pisa, Italy
2 Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Pisa, Largo Bruno Pontecorvo, 3, 56127 Pisa, Italy
Implementation of laser-plasma-based acceleration stages in user-oriented facilities requires the definition and deployment of appropriate diagnostic methodologies to monitor and control the acceleration process. An overview is given here of optical diagnostics for density measurement in laser-plasma acceleration stages, with emphasis on well-established and easily implemented approaches. Diagnostics for both neutral gas and free-electron number density are considered, highlighting real-time measurement capabilities. Optical interferometry, in its various configurations, from standard two-arm to more advanced common-path designs, is discussed, along with spectroscopic techniques such as Stark broadening and Raman scattering. A critical analysis of the diagnostics presented is given concerning their implementation in laser-plasma acceleration stages for the production of high-quality GeV electron bunches.
gas target interferometry laser-plasma laser wake-field acceleration Raman scattering Stark broadening 
High Power Laser Science and Engineering
2019, 7(2): 02000e26
Author Affiliations
Abstract
1 The Graduate School for the Creation of New Photonics Industries, 1955-1, Kurematsu, Nishiku, Hamamatsu, Japan
2 Faculty of Science and Engineering, Setsunan University, Neyagawa, 572-8508, Osaka, Japan
3 LULI-CNRS, Ecole Polytechnique, CEA: Universite Paris-Saclay, UPMC Univ Paris 06: Sorbonne Universites, F-91128, Palaiseau Cedex, France
4 Instituto de Fusion Nuclear, ETSI de Industriales, Universidad Politecnica de Madrid, C/ Jose Gutierrez Abascal, 2, E-28006, Madrid, Spain
5 LULI - CNRS, Ecole Polytechnique, CEA: Universite Paris-Saclay, UPMC Univ Paris 06: Sorbonne Universites, F-91128, Palaiseau Cedex, France
6 Department of Physics and Astronomy, University of California at Irvine, Irvine, CA, 92697, USA
The collective interaction between intense ion beams and plasmas is studied by simulations and experiments, where an intense proton beam produced by a short pulse laser is injected into a pre-ionized gas. It is found that, depending on its current density, collective effects can significantly alter the propagated ion beam and the stopping power. The quantitative agreement that is found between theories and experiments constitutes the first validation of the collective interaction theory. The effects in the interaction between intense ion beams and background gas plasmas are of importance for the design of laser fusion reactors as well as for beam physics.
Two stream instabilities Two stream instabilities Ultra intense short pulse laser Ultra intense short pulse laser Proton beam Proton beam Wake field Wake field Electron plasma wave Electron plasma wave Laser plasma interaction Laser plasma interaction 
Matter and Radiation at Extremes
2018, 3(3): 127
作者单位
摘要
郑州工业应用技术学院信息工程学院, 河南 新郑 451150
应用多光子非线性Compton 散射模型和数值模拟方法, 研究了正弦三角超强激光等离子的尾场对正电子加速, 提出了将入射超强激光和非线性Compton 散射光作为等离子体尾场对正电子加速的新机制, 给出了正电子加速能量修正公式和数值模拟结果。结果表明:使用非对称正弦三角激光脉冲的等离子体尾场加速正电子优于对称正弦三角激光脉冲的尾场情况, 散射使非对称正弦三角耦合激光脉冲宽度和上升长度与下降长度之比缩小, 正电子获得的加速能量显著增大。这是因为正电子频率增大, 横向速度各向异性分布增强, 尾场限制了正电子横向加速能量, 导致正电子在激光传输方向加速能量增大。
非线性光学 等离子体 超强激光 尾场 耦合 正电子 多光子非线性Compton 散射 
激光与光电子学进展
2015, 52(3): 031901
Author Affiliations
Abstract
Department of Electrical Engineering, Technion-Israel Institute of Technology, Haifa 32000, Israel
We present the first steps of a design of the optimal parameters for a full Bragg X-Ray free electron laser (BX-FEL). Aiming towards a future source of coherent X-ray radiation, operating in the strong Compton regime, we envisage the system to be the seed for an advanced light source or compact medical X-ray source. Here we focus on the design of the accelerator parameters: maximum gradient, optimal accelerated charge, maximum efficiency, and ‘wake coefficient’, which relates to the decelerating electric field generated due to the motion of a charged-line or train of charged-lines. Specifically, we demonstrate that the maximum efficiency has optimal value and given the fluence of the materials, the maximum accelerated charge in the train is constant. These two results might be important in any future design.
Bragg wake-field Compton scattering energy conversion efficiency fluence light source medical accelerator 
High Power Laser Science and Engineering
2014, 2(3): 03000e24
作者单位
摘要
1 中国工程物理研究院 激光聚变研究中心, 四川 绵阳 621900
2 清华大学 工程物理系, 北京 100084
激光尾波场加速伽玛射线源有望成为新一代小型强伽玛射线源。这种射线源具有高能量、高亮度、小焦斑、超短脉冲输出等特点。利用Geant4蒙特卡罗软件包, 计算了高能尾波场加速电子在高原子序数靶上的轫致辐射谱, 同时在轫致辐射谱的范围内, 计算了几种常用伽玛探测晶体相对发光效率和点扩展函数, 分析了它们与晶体厚度、材料及入射伽玛能量之间的关系, 为将来伽玛探测器的设计提供了理论参考。
伽玛射线源 激光尾波场 发光效率 点扩展函数 成像探测器 gamma source laser wake field scintillation efficiency point spread function imaging detector 
强激光与粒子束
2011, 23(5): 1378
作者单位
摘要
中国科学院 电工研究所,北京 100190
为了研究尾场效应引起的束流不稳定性,建立了由非对称Blumlein脉冲形成线、导体层和微堆层构成的介质壁加速器单元模块模型,用有限积分法对强流电子束在此结构中产生的尾场进行了计算,分别计算单组元和2组单元加速模块中的尾场势和尾场阻抗。从模拟的结果来看,x,y方向的尾场势和尾场阻抗都很小,束流尾场对横向的影响比较小。z方向的尾场势和尾场阻抗影响较大,尾场阻抗达到100 Ω量级。证明了由于介质壁加速器结构在加速腔长度和束流通过路径的连续性方面都具有很大的优势,横向阻抗小,束流尾场效应在束流不稳定性方面的影响相对较小,束流传输时的要求也会降低。
介质壁加速器 尾场 尾场势 尾场阻抗 有限积分法 dielectric wan accelerator wake field wake potential wake impendance finite integral method 
强激光与粒子束
2010, 22(4): 909
作者单位
摘要
1 美国弗吉尼亚大学物理系,弗吉尼亚,夏洛茨维尔,VA22904-4714
2 电力中央研究所,日本,东京,201-8511
用一维相对论粒子模拟研究了相对论超短强激光脉冲在等离子体中传播时激发的尾波场,初步获得了近共振区尾波场的峰值幅度随激光脉冲宽度变化的特点,发现在近共振区等离子体波激发出现增强.通过准静态近似下尾波激发的一维非线性方程数值求解,并与粒子模拟结果比较,得到了该非线性方程的适用范围:当激光脉冲宽度小于等离子体波波长的4倍时,该方程所得结果与粒子模拟结果一致;而当激光脉冲宽度大于该数值时,该方程不再适用.
超短强激光 等离子体尾波场 近共振 Ultrashort intense laser Plasma wake field Near resonant 
强激光与粒子束
2005, 17(5): 689
作者单位
摘要
1 中国工程物理研究院流体物理研究所,四川绵阳,621900
2 清华大学 加速器实验室,北京,100084
在理论分析的基础上,开发了直线感应加速器束流崩溃不稳定性数值模拟程序.描述了利用该程序开展的研究工作,这些研究揭示了束流崩溃不稳定性的一般规律,分析了相关参数对束流崩溃不稳定性的影响,最后提出了直线感应加速器束流崩溃不稳定性抑制方法.
直线感应加速器 束流崩溃不稳定性 横向阻抗 横向尾场 质心横向位移 数值模拟 Linear induction accelerator Beam breakup unstability Transverse impedance Transverse wake field Centroidal transverse displacement Numerical simulation 
强激光与粒子束
2003, 15(4): 397
作者单位
摘要
中国科学院上海光学精密机械研究所强光光学开放实验室,上海,201800
研究了在稀薄等离子体中强激光激发尾波场的情况,发现尾波场的激发与入射激光的脉冲宽度有共振现象.在光强很小情况下,共振所需要的入射激光脉冲宽度为??λ????p/2,随着光强的增大共振激光脉冲宽度减小.同时发现在稀薄等离子体中激发的尾波势场与等离子体的密度几乎无关,而激发的尾波场最大电场强度与等离子体的密度有关.
稀薄等离子体 尾波场 共振条件 
光学学报
2002, 22(2): 157
作者单位
摘要
中国科学技术大学,国家同步辐射实验室,安徽,合肥,230029
根据同轴线方法测量阻抗的原理,用模拟方法讨论了该测量方法的有效性问题.从均匀圆波导和同轴线结构中的电磁场解析分析,说明了该方法有效性问题的起源和基本物理图像,简单回顾其他方法讨论该问题的结论,最后数值模拟分析了同轴线方法测量束流耦合阻抗的有效性,所得主要结论能够对阻抗测量平台的设计提供可靠的依据.
尾场 耦合阻抗 同轴线方法 传输特性参数 wake field coupling impedance coaxial wire method transmission parameter 
强激光与粒子束
2002, 14(6): 920

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