共查询到18条相似文献,搜索用时 125 毫秒
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研究了紧聚焦的圆偏振飞秒相对论高斯激光脉冲与电子的相互作用,提出了一种激光加速电子的新机制.利用束腰小、强度大的激光脉冲上升沿加速电子,束腰大、强度小的脉冲下降沿减速电子,当光脉冲和电子分离时,电子获得了能量增益.研究发现,初始静止的电子与强度高于1019Wμm2/cm2的光脉冲作用以后,可以获得MeV量级的能量.初始位于焦点附近的电子被加速的效果较好,而远离焦点的电子几乎不能获得能量增益.
关键词:
电子加速
能量增益
高斯脉冲
束腰 相似文献
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通过求解电子运动的相对论方程,发现预加速电子在超强超短激光脉冲的作用下可以获得很高的能量增益. 飞秒激光脉冲的上升沿在焦点附近的区域有效加速电子后,电子和光脉冲一起传播一段距离(远大于瑞利长度)后,激光强度变得很弱,从而使脉冲下降沿对电子的减速作用可以忽略不计,因此电子只经历加速过程而没有被减速,当电子和光脉冲分离时,电子获得了很高的能量增益. 当光强为1019W/cm2 ,电子的初始能量为MeV量级时,电子的能量增益可以达到01GeV. 进一步讨论了电子的能量增益与电子的初始条件与激光脉冲的参数之间的关系.
关键词:
电子加速
飞秒激光脉冲
能量增益 相似文献
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室温,常压下,利用Nd∶YAG脉冲激光器产生的波长为1 064 nm, 脉宽12 ns,能量分别180, 230和280 mJ的脉冲激光冲击Ti靶,使用中阶梯光栅光谱仪检测了三种激光能量下对应的光谱。调节延时器DG645的延迟时间,检测了延迟0~500 ns时间范围内Ti等离子体对应激光能量下的发射光谱,分析光谱,可以得到了九条不同的的TiⅠ 和TiⅡ等离子体谱线,证明在该实验条件下,Ti靶能够充分吸收能量电离且离子谱线具有不同的演化速率,利用Saha-Boltzmann法计算并分析Ti等离子体电子温度,实验结果表明:相同的延迟时间,激光能量越大,谱线相对强度越大,电子温度越高,谱线相对强度的变化量随激光能量的变化量增大而增大;在延时0~150 ns内,三种激光能量下的等离子体电子温度和谱线的相对强度都随延迟时间的增加而快速下降,其中280 mJ激光能量下的等离子体电子温度和谱线强度下降速率较快;在150~250 ns范围内,电子温度和谱线强度均随延迟时间的增加有一个缓慢的上升,180 mJ激光能量下的等离子体电子温度和谱线强度的上升速率较快。250~500 ns范围内,三种激光能量下的电子温度和谱线强度均随延迟时间的增加而缓慢下降。 相似文献
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利用非线性汤姆孙散射的理论,从理论和数值模拟上研究了单电子在横向穿越高斯激光束束 腰时所辐射的x射线阿秒脉冲列的性质. 主要分析了电子以初始能量γ0=1M eV—100M eV横向穿越激光振幅参数为a0=1—10的高斯光束束腰获得的阿秒辐射脉冲的 时间 和空间性质. 计算表明,辐射呈现脉冲列的形式. 脉冲列的包络宽度取决于激光强度、束腰 的宽度以及入射电子能量. 电子的初始能量比激光强度对电子辐射脉冲的影响更大. 辐射脉 宽、脉冲间隔和脉冲包络宽度都正比于1/γ20,辐射功率正比于 γ60,辐射能 量正比于γ40. 当改变激光振幅a0时,辐射功率正比 于a20、辐射包络中单 个脉冲脉宽正比于1/a0、脉冲之间的间隔正比于a0. 当保持激光强 度不变,而改变光束 束腰半径w0时,辐射的脉冲数量、包络和辐射能量正比于w0. 当 激光功率保 持不变时而改变激光强度和束腰半径时,脉冲包络宽度和最大辐射能量都基本不变. 当激光 振幅参数a0=1,电子初始能量为10MeV时,激光束腰为两个激光波长时,电子 辐 射脉冲包络宽度只有14×10-3τ0(τ0为入 射激光周期),达到几个阿秒的量级.
关键词:
阿秒脉冲
非线性汤姆孙散射
高斯激光光束 相似文献
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采用解析方法,在考虑材料损耗和色散的情况下,详细研究了无啁啾高斯脉冲和啁啾高斯脉冲在半导体光放大器中传输的物理过程,分析了强度增益、脉冲宽度和频率啁啾与线宽增强因子、色散系数、小信号增益特征参数及初始啁啾之间的关系。结果表明:当输入变换极限的高斯脉冲时,色散会引起增益压缩,脉冲展宽和频率啁啾;同样情况下,线宽增强因子越大,脉宽加宽越明显,输出脉冲啁啾越大,且随着线宽增强因子的增大,输出脉冲啁啾极大值向特征参数值较小的一边移动。当输入啁啾高斯脉冲时,初始脉冲啁啾越大,增益压缩越明显,啁啾系数为正时,脉冲单纯展宽,输出啁啾随特征参数的增大而逐渐减小,啁啾系数为负时,初始啁啾与群速度色散导致的啁啾相互竞争,致使脉冲先被压缩后被展宽;脉冲最窄处对应的特征参数随线宽增强因子的增大而先增大后减小,输出啁啾随特征参数的增大而经历振荡后趋于平稳。 相似文献
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使用粒子模拟程序对30 fs超短超强激光在均匀与抛物型两种密度分布等离子体中的传输, 以及在稳定传输状态下尾场的电子注入与加速形成的电子能谱进行了模拟与分析. 固定入射激光束斑尺寸, 在(0.4-2)×1019/cm3等离子体密度范围, 对比分析了归一化峰值强度从1-6范围的激光脉冲在上述两种密度分布等离子 体中传输时激光束斑尺寸的演化, 结果表明抛物型分布的等离子体密度通道能够对超短超强脉冲实现良好的导引, 有利于高能电子加速. 对于较高密度情况,即使在均匀等离子体中依靠相对论自聚 焦等机制也可以实现良好的自导引传输,有利于实验简化以及产生更大电量的加速电子. 相似文献
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HE Feng YU Wei LU Pei-Xiang XU Han SHEN Bai-Fei QIAN Lie-Jia LI Ru-Xin XU Zhi-Zhan 《理论物理通讯》2005,43(5):910-914
With the development of photocathode rf electron gun, electrons
with high-brightness and mono-energy can be obtained easily. By
numerically solving the relativistic equations of motion of an
electron generated from this facility in laser fields modelled by
a circular polarized Gaussian laser pulse, we find the electron
can obtain high energy gain from the laser pulse. The corresponding acceleration distance for this electron driven by the ascending part of the laser pulse is much longer than the
Rayleigh length, and the light amplitude experienced on the
electron is very weak when the laser pulse overtakes the electron.
The electron is accelerated effectively and the deceleration can
be neglected. For intensities around 1019 W•μm2/cm2, an
electron's energy gain near 0.1 GeV can be realized when its
initial energy is 4.5 MeV, and the final velocity of the energetic
electron is parallel with the propagation axis. The energy gain
can be up to 1 GeV if the intensity is about 1021 W•μm2/cm2. The final energy gain of the electron as a function of its initial conditions and the parameters of the laser beam has
also been discussed. 相似文献
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Yu. E. Geints A. A. Zemlyanov 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2009,55(3):745-754
Focused propagation of high-power femtosecond laser radiation in air is
considered. Based on numerical solution of the nonlinear Schr?dinger
equation for complex envelope of light wave electric field, evolution of the
beam effective radius is studied. The dependence of the effective (rms) size
of a focal spot and the maximally achievable intensity of laser radiation at
focal waist on the initial pulse power is established. It is shown that
focal spot of tightly focused intensive ultrashort laser radiation can
change its size during the pulse passage through the beam waist. This is the
consequence of pulse intensity clamping in region of beam focusing caused by
gas photoionization and plasma producing. This may prevent laser intensity
from its further growth in the focal region and arrest the transversal
compression of the beam in the linear focus as a whole. 相似文献
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Intense laser beam guiding in self-induced electron cavitation channel in underdense plasmas 下载免费PDF全文
In underdense plasmas, the transverse ponderomotive force of an
intense laser beam with Gaussian transverse profile expels electrons
radially, and it can lead to an electron cavitation. An improved
cavitation model with charge conservation constraint is applied to
the determination of the width of the electron cavity. The envelope
equation for laser spot size derived by using source-dependent
expansion method is extended to including the electron cavity. The
condition for self-guiding is given and illuminated by an effective
potential for the laser spot size. The effects of the laser power,
plasma density and energy dissipation on the self-guiding condition
are discussed. 相似文献
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Propagation of an intense short laser pulse through under-dense plasma can produce huge amplitude plasma wake field. A 3D particle in cell (PIC) method was used to simulate the wakefield generation for different laser parameters such as intensity, pulse duration, spot size and temporal pulse shape. Our study shows that the amplitude of wakefield is increased with laser intensity, but it is decreased with spot size. The results for pulse shape and pulse duration depend on their optimum values. 相似文献
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Particle simulation on electron acceleration process by the laser ponderomotive force in inhomogeneous underdense plasma layers 下载免费PDF全文
The mechanism of electron ponderomotive acceleration due to increasing group velocity of laser pulse in inhomogeneous underdense plasma layers is studied by two-dimensional relativistic parallel particle-in-cell code. The electrons within the laser pulse move with it and can be strongly accelerated ponderomotively when the duration of laser pulse is much shorter than the duration of optimum condition for acceleration in the wake. The extra energy gain can be attributed to the change of laser group velocity. More high energy electrons are generated in the plasma layer with descending density profile than that with ascending density profile. The process and character of electron acceleration in three kinds of underdense plasma layers are presented and compared. 相似文献
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研究表明, 峰值强度为1022–1025 W/cm2量级的圆偏振激光脉冲的有质动力场可以直接加速并产生GeV–TeV的单能电子束, 其中被加速电子的能量与激光脉冲的峰值强度成线性定标关系. 为了获得更高能量的电子束, 通过对一维解析模型的分析得到: 如果电子束在激光传播的方向上具一个初始能量E0, 那么这种线性的定标关系可以被打破, 被加速电子束最终的能量可以被放大E0倍. 这是由于具有一定初始能量的电子束不容易被激光脉冲抛在后面, 进而获得更高的加速距离. 二维粒子模拟结果显示: 当电子束的初始能量E0为MeV量级时这个方法是有效的, 而当E0过大时这个方法失效. 这是因为当电子的加速距离远大于激光脉冲的瑞利长度时, 激光强度的衰减使得电子束的加速错过了最佳加速场. 相似文献