自由电子激光放大啁啾脉冲的数值模拟

利用1维非定态程序对单程自由电子激光(FEL)放大器放大线性啁啾脉冲的过程进行了数值模拟,得到了不同啁啾参数的脉冲通过FEL放大器的增益曲线,计算了不同啁啾参数的脉冲被单程FEL放大器放大后的腔外压缩情况。通过对数值模拟结果的定性分析得出：影响输出脉冲宽度和峰值功率的主要因素是FEL放大器的增益线宽和啁啾参数,并以此说明,通过先使用FEL放大器放大啁啾脉冲、然后再将其在腔外压缩的方法产生超短脉冲FEL是可行的。     

能量啁啾电子束自由电子激光放大啁啾脉冲

 提出采用具有能量啁啾电子束的自由电子激光放大器放大啁啾脉冲,分析说明了它的工作机理和滑移现象对其的影响。采用研制的1维非定态程序GOFEL-P,对能量啁啾自由电子激光放大器放大啁啾脉冲的过程进行了数值模拟和分析,计算了不同啁啾参数的脉冲被放大后的腔外压缩情况。结果表明：与单能电子束时相比,能量啁啾自由电子激光可以放大具有更大啁啾参数的啁啾脉冲,使压缩后的脉冲峰值功率增大至568 GW,脉冲宽度缩短至2.29 fs,大幅增强自由电子激光放大啁啾脉冲以及腔外压缩脉冲的效果。     

短波自由电子激光放大器数值模拟

介绍在理论上研究自由电子激光(FEL)的MICFEL程序。MICEFL是以单粒子理论为基础的二维放大器程序。利用MICFEL计算的Paladin实验结果与FRED程序计算结果以及25米Paladin实验结果相比均基本符合。理论计算的结果显示了FEL增益光导的特性。     

自由电子激光三维数值模拟

在不降低计算精度条件下,保持FELEX程序的基本框架,我们采用了自接法,变量变换,制表等一系列改进措施,使自由电子激光三维模拟计算缩短了一到二个量级的CPU时间,并在PC386/25上实现了运行程序。     

自由电子激光振荡器的二维数值模拟

在柱二维坐标系中,用数值计算方法求解了摇摆器内电子模拟方程组、光场方程组和无源区(不含摇摆器区)经非自适应方法变换后的无源旁轴波动方程并设计了相应的程序R_2D。用该程序计算的数值结果表明,在有源条件下二维数值模拟结果与高斯光束近似下的数值模拟结果符合较好;取完全相同的计算条件R-2D程序与洛斯阿拉莫斯实验室(LANL)的FELEX程序的计算结果符合较好;初步认为LANL实验数据的物理图象合理,数值结果基本可信;最后给出北京自由电子激光器(BFEL)的一些物理数据。     

自由电子激光光导的数值模拟与分析

从一维自由电子激光理论出发,唯象地考虑衍射效应,计算和分析了光导效应的特点和规律;针对曙光一号装置的自由电子激光参数,利用二维理论对光场剖面、填充因子、光场半径等进行了数值模拟;根据计算结果分析和讨论了影响光导的因素和实验条件。     

自由电子激光振荡器的三维数值模拟

仔细地考查了与三维自由电子激光振荡器物理方程组相应的３－Ⅰ程序的可靠性。在此基础上使用该程序计算、分析了在电子束与光束同轴条件下，当电子束参数如能散度、发射度、束流等参量改变时三维自由电子激光的一些基本规律。     

增益饱和在整形放大啁啾脉冲中的作用

根据线性啁啾脉冲的特点，利用增益介质的受激发射谱特性，及脉冲在饱和放大时的放大特点，从理论上提出一种获得强度分布前后沿对称放大啁啾脉冲输出的方法，并利用数值模拟对该方法的可行性进行了研究，具体给出了在利用该种方法产生强度前后沿对称的放大啁啾脉冲输出时，应该遵循的部分规律。     

毫米波圆柱波导自由电子激光放大器的数值模拟

本文以单粒子理论为基础，在不计空间电荷效应的近似条件下推导了带轴向引导磁场的三维圆柱波导非线性模拟方程组。用CAGFEL程序计算、分析了在带入口区、常数摇摆器条件下两组不同物理参数的自由电子激光放大器的物理模型。计算结果可靠，物理图象合理。对于其中的第二组参数还着重考查了光波频率、输入功率和摇摆器场振幅改变对输出功率和效率的影响。上述这些计算结果对0．7MeV 自由电子激光放大器的设计和实验具有一定的参考价值。     

自由电子激光同步振荡边带超辐射的数值模拟研究

给出了描述自由电子激光同步振荡边带超辐射的方程组和它的解法,用编制的数值计算程序,对系统进行数值模拟研究,给出边带超辐射的频率和功率的定量结果,并证明在边带辐射中诱导辐射仍是主要的。     

Numerical analysis of spatial distortions in a single-grating chirped pulse amplification system

A numerical study of spatial distortions of a laser beam after propagation through an optical single-grating chirp pulse amplification (CPA) system was developed. This study is based on numerical simulation using the ray-tracing model from Rayica module of MATHEMATICA and it relates the behavior of the aberrated beam in terms of spatial distortions (eg. spatial chirp and pulse front tilt) in case of grating incident angle variation. The results are relevant for different applications which use CPA systems with needs of high quality laser beam profile.     

Mutual compensation of higher-order dispersion in chirped pulse amplification system with regenerative amplifier

In this paper, based on ray tracing, the approach of mutual compensation that introduced properly the negative third-order dispersion to balance the higher-order dispersion in the chirped pulse amplification (CPA) system with regenerative amplifier is presented. A shorter pulse with near-transform-limitation can be generated by this method than by the conventional approach that zeros the second- and the third-order dispersion successively in the CPA system.     

Numerical studies of optical parametric chirped pulse amplification

Based on the coupled wave equations, optical chirped-pulse parametric amplification (OPCPA) is simulated and its characteristics are investigated under the conditions of small-signal and pump depletion. The influence of the group-velocity mismatch and the phase mismatch among the three waves on the process of the amplification are discussed, respectively. Compared with the conventional chirped-pulse amplification system, synchronization between pump and signal-pulses is a crucial issue in OPCPA. The requirement on Δτ_p–s as well as the stability of the system is investigated.     

Parametric amplification of chirped optical pulses under pump depletion

We present simple analytical solutions of coupled wave equations describing chirped pulse parametric amplification under pump depletion. The evolution of the duration and spectrum of amplified pulses in OPA pumped by Gaussian and supergaussian pulses has been investigated both numerically and analytically. Also, the dependence of the energy conversion efficiency from pump to signal was determined for a range of parameter values, and an optimum ratio of signal and pump pulse durations was evaluated.     

啁啾脉冲参量放大特性的数值模拟研究

 根据啁啾脉冲激光参量放大技术,数值模拟了光参量放大在啁啾脉冲放大中的应用。研究啁啾脉冲参量放大增益及时间特性,特别是在大信号注入与小信号注入两种有代表意义的情况下,详细地分析了群速度失配、相位失配对放大过程的影响。研究了泵浦光脉冲与信号光脉冲的时间同步要求,讨论了放大系统的稳定性。     

SASE自由电子激光起振问题及统计特性的数值模拟

 介绍一种自放大自发辐射自由电子激光（SASE FEL）的自发辐射和电子束噪声的数学描述，运用修正的一维非定态程序，对SASE FEL 起振问题及光场统计特性进行了数值模拟，分析了自发辐射谱的发展过程及一定频带宽度内光场随机特性的统计规律，数值模拟结果与理论结果符合较好。     

SASE自由电子激光起振问题及统计特性的数值模拟

介绍一种自放大自发辐射自由电子激光（SASE FEL）的自发辐射和电子束噪声的数学描述,运用修正的一维非定态程序,对SASE FEL 起振问题及光场统计特性进行了数值模拟,分析了自发辐射谱的发展过程及一定频带宽度内光场随机特性的统计规律,数值模拟结果与理论结果符合较好。     

Fiber based high repetition rate, high energy laser source applying chirped pulse amplification

We demonstrate the potential of a high-gain Yb-fiber amplifier system to provide ultrashort pulses with high energies. 100 μJ pulses generated at a repetition rate of 32 kHz exhibit nearly diffraction limited output (M²≈1.7) at a 1060 nm center wavelength. Using chirped pulse amplification, temporally streched laser pulses from a femtosecond oscillator could be compressed after amplification to subpicosecond pulse duration. The achievable intensities are high enough to create plasmas which can efficiently convert laser light to the extreme ultraviolet radiation. In a multimode Yb-doped fiber amplifier we obtained average powers of up to 22 W and single pulse energies up to 130 μJ.     

Stacking chirped pulse optical parametric amplification

Stacking chirped pulse optical parametric amplification based on a home-built Yb³⁺-doped mode-locked fiber laser and an all-fiber pulse stacker has been demonstrated. Energic 11 mJ shaped pulses with pulse duration of 2.3 ns and a net total gain of higher than 1.1 × 10⁷ at fluctuation less than 2% rms are achieved by optical parametric amplification pumped by a Q-switched Nd:YAG frequency-doubled laser, which provides a simple and efficient amplification scheme for temporally shaped pulses by stacking chirped pulse.