朱军高 1卢海洋 3,*赵媛 3赖美福 3[ ... ]周沧涛 3,***
作者单位
摘要
1 深圳大学 应用技术学院 深圳 518060
2 深圳市微纳光子信息技术重点实验室,教育部/广东省共建光电子器件和系统重点实验室,深圳大学物理与光电工程学院 深圳 518060
3 深圳技术大学 工程物理学院 先进材料测试技术研究中心,深圳市超强激光与 先进材料技术重点实验室 深圳 518118
4 湖北大学 物理与电子科学学院 武汉 430062
激光等离子体加速输出的电子束具有fs量级脉冲长度的优异品质。由于强激光场的存在,直接应用存在一定困难,更多应用场景需要把电子束传输到应用端。能散导致电子束在传输中产生能量啁啾,需要通过束流光学设计抑制脉冲长度的增长。通过对电子束在消色差束线中传输的研究,探索了消色差和非消色差传输中脉冲长度压缩的差异,以及消色差束线中偏转角度、偏转半径对不同能量电子束脉冲长度压缩的影响。针对消色差传输中仅有某个能量电子束得到最优压缩的局限,利用四极透镜磁场梯度的调节使电子束的传输适度偏离消色差,改变对能量啁啾的影响,实现在固定尺寸束线中不同能量电子束的压缩。
激光加速 电子束传输 电子束应用 超快 Laser acceleration Electron beam transmission Electron beam application Ultrafast 
核技术
2023, 46(2): 020201
Author Affiliations
Abstract
1 Center for Advanced Material Diagnostic Technology and College of Engineering Physics, Shenzhen Technology University, Shenzhen 518118, People’s Republic of China
2 Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Shenzhen Technology University, Shenzhen 518118, People’s Republic of China
3 College of Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, People’s Republic of China
We present a novel scheme for dense electron acceleration driven by the laser irradiation of a near-critical-density plasma. The electron reflux effect in a transversely tailored plasma is particularly enhanced in the area of peak density. We observe a bubble-like distribution of re-injected electrons, which forms a strong quasistatic electromagnetic field that can accelerate electrons longitudinally while also preserving the electron transverse emittance. Simulation results demonstrate that over-dense electrons could be trapped in such an artificial bubble and accelerated to an energy of 500MeV. The obtained relativistic electron beam can reach a total charge of up to 0.26 nC and is well collimated with a small divergence of 17 mrad. Moreover, the wavelength of electron oscillation is noticeably reduced due to the shaking of the bubble structure in the laser field. As a result, the energy of the produced photons is substantially increased to the γ range. This new regime provides a path to generating high-charge electron beams and high-energy γ-ray sources.
Matter and Radiation at Extremes
2023, 8(1): 014403
作者单位
摘要
1 深圳技术大学 工程物理学院,先进材料测试技术研究中心,深圳市超强激光与先进材料技术重点实验室,广东 深圳 518118
2 深圳大学物理与光电工程学院,深圳市微纳光子信息技术重点实验室,教育部/广东省共建光电子器件和系统重点实验室,广东 深圳 518060
激光加速器可以输出具有独特品质的质子束,例如µm尺寸、ps脉冲长度和高峰值电流。强流粒子束的空间电荷力效应较强,对面向应用的束流传输提出了挑战。通过二维PIC模拟研究了激光加速后与质子速度接近的电子的影响。采用椭球模型估算空间电荷力的影响,比较不同电荷分布的差异。结果表明每束团质子数超过1010后空间电荷力显著影响质子束传输,甚至严重破坏束流品质。空间电荷力的影响在20 ps后显著减弱,离开靶约1.2 mm。
激光加速 质子束 空间电荷力 高亮度 laser acceleration proton beam space charge force high brightness 
强激光与粒子束
2023, 35(2): 021004
作者单位
摘要
1 北京大学 核物理与核技术国家重点实验室,北京 100871;北京怀柔激光加速创新中心,北京 101407
2 北京大学 核物理与核技术国家重点实验室,北京 100871;北京大学 应用物理研究中心,北京 100871
3 北京大学 核物理与核技术国家重点实验室,北京 100871;北京怀柔激光加速创新中心,北京 101407;北京大学 应用物理研究中心,北京 100871
激光离子加速是近年来激光等离子体领域兴起的研究热点之一。激光产生的高能离子束具有高亮度、小尺寸、脉宽窄和方向性好等特点,具有很多潜在的应用。概述了几种常见的激光离子加速物理机制,对一系列激光离子加速实验进展进行了归纳总结,最后介绍了几种激光驱动离子束的潜在应用。
激光等离子体 粒子加速 超短激光 超强激光 laser plasma particle accelerator ultra-short laser ultra-intense laser 
强激光与粒子束
2020, 32(9): 092002
作者单位
摘要
北京大学核物理与核技术国家重点实验室, 北京 100871
在北京大学200 TW激光系统上,测量了经可编程声光色散滤波器不同程度光谱调制后放大器输出脉冲的频域分布,并设计了一个与脉冲中心波长、光谱宽度等参数相关的光谱调制函数拟合了实验测得的光谱数据。该函数形式简单,适用于不同的激光系统。对实验系统中种子脉冲经光谱调制后从放大器输出的光谱结果进行了数值模拟,对比研究了普通种子脉冲和光谱调制脉冲经放大器增益后时域空间内的物理性质;讨论了光谱调制对系统最终输出脉冲峰值功率的影响。结果表明:光谱调制会导致脉冲旁瓣的产生,降低系统输出脉冲的有效能量和飞秒对比度,系统输出脉冲为平顶光谱时,其有效输出峰值功率最大。
超快激光 时域特性 调制函数 光谱调制 
中国激光
2017, 44(5): 0501001
作者单位
摘要
北京大学 核物理与核技术国家重点实验室, 北京 100871
介绍一种使用闪烁体耦合电子倍增电荷耦合器件(EMCCD)的方式对离子进行记录的汤姆逊能谱仪,可实现对离子能谱的实时单发测量。同时,该谱仪利用倾斜电极板对离子进行偏转,可减少由于离子打在电极板上产生的电磁噪声,能够提高实验结果的信噪比。该谱仪在北京大学4.5 MV静电加速器和2×6 MV串列加速器上进行了标定实验,测量了闪烁体将离子转化成光子后的探测效率,实验结果也验证了该谱仪的可行性和稳定性。该汤姆逊谱仪将用于北京大学激光加速器CLAPA对离子束流的测量研究。
汤姆逊离子谱仪 激光离子加速 离子能谱测量 Thomson spectrometer laser-driven ion acceleration ion spectrum analysis 
强激光与粒子束
2015, 27(11): 112001
Author Affiliations
Abstract
In this letter, we discuss the increase in the average cluster size by lowering the stagnation temperature of the methane (CH4) gas. The Coulomb explosion experiments are conducted to estimate the cluster size and the size distribution. The average CH4 cluster sizes Nav of 6 230 and 6 580 are acquired with the source conditions of 30 bars at 240 K and 60 bars at 296 K, respectively. Empirical estimation suggests a five-fold increase in the average size of the CH4 clusters at 240 K compared with that at room temperature under a backing pressure of 30 bars. A strong nonlinear Hagena parameter relation (\Gamma *\propto T^{-3.3}) for the CH4 clusters is revealed. The results may be favorable for the production of large-sized clusters by using gases at low temperature and high back pressures.
020.2649 Strong field laser physics 350.5400 Plasmas 
Chinese Optics Letters
2013, 11(s2): S20201
Author Affiliations
Abstract
We present three possible design options of laser plasma acceleration (LPA) for reaching a 100-GeV level energy by means of a multi-petawatt laser such as the 3.5-kJ, 500-fs PETawatt Aquitane Laser (PETAL) at French Alternative Energies and Atomic Energy Commission (CEA). Based on scaling of laser wakefield acceleration in the quasi-linear regime with the normalized vector potential a0 = 1.4(1.6), acceleration to 100 (130) GeV requires a 30-m-long plasma waveguide operated at the plasma density ne \approx 7 \times 10^{15} cm^{ 3} with a channel depth \Delta n/ne=20%, while a nonlinear laser wakefield accelerator in the bubble regime with a0 \geq 2 can reach 100 GeV approximately in a 36/a0-m-long plasma through self-guiding. The third option is a hybrid concept that employs a ponderomotive channel created by a long leading pulse for guiding a short trailing driving laser pulse. The detail parameters for three options are evaluated, optimizing the operating plasma density at which a given energy gain is obtained over the dephasing length and the matched conditions for propagation of relativistic laser pulses in plasma channels, including the self-guiding. For the production of high-quality beams with 1%-level energy spread and a 1\pi-mm-mradlevel transverse normalized emittance at 100-MeV energy, a simple scheme based on the ionization-induced injection mechanism may be conceived. We investigate electron beam dynamics and effects of synchrotron radiation due to betatron motion by solving the beam dynamics equations on energy and beam radius numerically. For the bubble regime case with a0=4, radiative energy loss becomes 10% at the maximum energy of 90 GeV.
350.4990 Particles 350.5400 Plasmas 
Chinese Optics Letters
2013, 11(1): 013501
Author Affiliations
Abstract
State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800
We use an electrostatic model to study the average kinetic energy of ions ejected from the pure Coulomb explosions of methane clusters (CA4)n (light atom A=H and D). It is found that the ratio of the average kinetic energy of the ions to their initial average electrostatic potential energy is irrelevant to the cluster size. This finding implies that as long as the ratio is given, the average kinetic energies of the ions can be simply estimated from their initial average electrostatic potential energies, rather than from the time-consuming simulations. The ratios for the different charge states of carbon ions are presented.
甲烷团簇 纯库仑爆炸 离子平均动能 020.0020 Atomic and molecular physics 320.2250 Femtosecond phenomena 
Chinese Optics Letters
2008, 6(6): 391

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