电磁波泵浦的自由电子激光器

本文研究了电磁波泵浦的自由电子激光器。从跃变磁场结构出来的大半径迴旋环形电子束通过圆柱形波导与圆柱形波导的TE11模入射电磁波相作用。利用电子束的弗拉索夫分布函数理论和三维波导模的波动方程求得在康普顿区域中的散射波色散关系。通过数值分析,讨论了轴向引导磁场,电子束能量,电子迴旋比和电子束环的径向位置等与散射波频率和增长率的关系。     

损耗介质加载结构Ka波段TE_(01)模回旋行波管放大器稳定性的分析

该文从分析损耗介质加载金属圆波导中电磁波传输特性出发,应用回旋行波管放大器小信号色散方程,研究损耗介质加载结构TE01模回旋行波管放大器绝对不稳定性振荡和回旋返波振荡对器件稳定性的影响.结果表明:损耗介质的加载,可以提高绝对不稳定性起振电流,提高的幅度依赖于工作磁场偏离饱和磁场的程度、电子束横纵速度比等;增加波导损耗介质加载的厚度,可以提高竞争模式的回旋返波起振长度.合理选择波导的损耗层厚度、介电常数以及回旋行波管的工作电压、工作磁场和电子束横纵速度比,可以有效兼顾带宽和抑制不稳定性,保证回旋行波管放大器稳定工作.     

损耗介质加载结构Ka波段TE01模回旋行波管放大器稳定性的分析

该文从分析损耗介质加载金属圆波导中电磁波传输特性出发,应用回旋行波管放大器小信号色散方程,研究损耗介质加载结构TE₀₁模回旋行波管放大器绝对不稳定性振荡和回旋返波振荡对器件稳定性的影响。结果表明：损耗介质的加载,可以提高绝对不稳定性起振电流,提高的幅度依赖于工作磁场偏离饱和磁场的程度、电子束横纵速度比等;增加波导损耗介质加载的厚度,可以提高竞争模式的回旋返波起振长度。合理选择波导的损耗层厚度、介电常数以及回旋行波管的工作电压、工作磁场和电子束横纵速度比,可以有效兼顾带宽和抑制不稳定性,保证回旋行波管放大器稳定工作。     

用波导激光理论讨论自由电子激光辐射的传输

本文提出新的建议,用波导激光理论来处理自由电子激光辐射的传输问题。研究表明,存在特定的低损耗传输模。介质波导中电磁场为EH_(11)模。讨论了模的耦合损耗。     

考虑纵向动量离散的离子波纹激光动力学理论

利用动力学理论对一种新型自由电子激光－离子波纹激光（ＩＲＬ）进行了研究。考虑电子束的纵向动量离散和空间电荷场效应，导出了ＩＲＬ不稳定性色散关系，求得了ＩＲＬ辐射波的增长率及电子束空间电荷波的线性阻尼率，并对其进行了讨论，得到了一些结论。     

考虑了波导宽壁糟和金属鳍厚度效应的鳍线特性研究

本文全波分析了考虑波导宽壁槽和金属鳍厚度效应的鳍线传输特性.给出了单侧和耦合单侧鳍线的理论计算曲线,与假定波导宽壁槽深和金属鳍厚度为零情形下的计算结果相比较,证明了在毫米波高频段,波导宽壁槽和金属鳍厚度对给线传输特性影响很大.     

有矩形波导和线性摆动器的自由电子激光器的特性研究

本文研究圆柱电子束通过矩形波导和线性摆动器时产生相干辐射的特性。用线性化弗拉索夫-麦克斯韦方程分析了因对自洽的电子束平衡态引起扰动产生的不稳定性。导出了TMmn模的色散方程并数值计算了辐射频率和增长率与电子束能量、轴向磁场、摆动器强度和波长以及电子束半径的关系。     

采用静电聚束的环形自由电子激光器

本文用线性理论研究了一种采用静电聚束系统和角向摆动场(Wiggler)的环形自由电子激光器,导出了自由电子激光不稳定性色散方程,并从此方程求得了最大自由电子激光不稳定性增长率。文中还就有关问题进行了讨论。     

纳米级铝包覆光波导耦合特性研究

为了研究10nm级铝包覆光波导特征参量对其耦合情况的影响,理论模拟了不同金属层折射率和厚度、不同导波层折射率和厚度情况下的衰减全反射谱,分析了特征参量对耦合情况的影响。通过实验验证了金属层折射率和厚度对其耦合情况的影响,发现纳米级铝膜的复介电常数发生了很大的变化。结果表明,导波层厚度影响激发导模的数目,但对耦合深度影响不大;导波层折射率同时影响激发导模的数目和耦合深度;耦合层金属膜厚度不影响激发导模的模数,但对耦合深度的影响很大;对于相同的耦合层金属膜厚度,金属折射率不同,耦合情况大不相同。研究结果为基于双面金属包覆光波导的脉冲展宽器的制作和设计过程提供了参考。     

光导波的声光布喇格偏转

光导波声光Bragg偏转器有可能应用于宽带射频信息的处理。本文介绍光导波声光Bragg偏转器的设计、制作与实验结果。 1.光波导结构与耦合 光波导基片为y切LiNbO_3,晶轴的x、y和z方向分别约为40毫米、2毫米和10毫米。GOW沿x轴传播,SAW沿z轴传播。基片表面经严格光学抛光。用电子束热蒸发在其表面沉积一层约300(?)厚的Ti膜,经1000℃氧气氛下扩散而成渐变折射率光波导。用一锗酸铋棱镜把He-Ne激光器的6328(?)光耦合到波导中,可分别激励TE模和TM模的各个模式,再用同样的棱镜将制导光束耦合出来。TK_o模穿透深度约为3微米,波导损耗约为2分贝/厘米。     

THE TRANSVERSAL GEOMETRIC EFFECTS IN A FREE ELECTRON LASER

The effects of a beam thickness and a conducting wall in a free electron laser with a linearlypolarized wiggler magnetic field and an axial magnetic field are investigated within the framework of fluid-Maxwell equations.The growth rate of free electron laser instability is obtained,in which the nonlinear bulkand surface current density are simultaneously considered.The numerical calculations indicate that the bulkcoupling is dominant.There is an optimum beam thickness and separation between the conducting walls forwhich the growth rate is maximum.     

Mode analysis of an open-boundary cerenkov laser in the collective regime

The mode analysis of an open-boundary Cerenkov laser is developed in the collective regime. The Cerenkov laser under consideration consists of a relativistic slab electron beam and a dielectric-loaded conducting plane. The beam and the dielectric are assumed to be arbitrary in thickness, with an arbitrary gap allowed between them. For the Cerenkov laser specified above, the dependence of the growth rate upon the electron density of the beam, the beam-dielectric gap, the beam thickness, and the drift velocity of the beam is clarified. In particular, the following results deserve special attention. First, with other parameters kept invariant, the growth rate approaches a constant value for the beam thickness greater than the reactive skin depth of the beam. Second, the growth rate becomes maximum at the drift velocity of the beam characteristic of a particular electromagnetic wave mode with which the space charge wave interacts. As the mode number increases, the characteristic drift velocity shifts to higher values whereas the value of the maximum growth rate decreases.     

Field theory of dielectric Cherenkov maser

The effect of three-dimensional perturbed velocity and three-dimensional perturbed current density on the beam-wave interaction of dielectric Cherenkov maser is analysed by use of the self-consistent linear field theory. Three distinct cases are considered. First, the propagation of the electron beam in an annular dielectric liner enclosed by a loss-free conducting wall is investigated. The dispersion equation and the simultaneous condition of the beam-wave interaction are derived. It's clearly shown that the instability of the interaction results from the coupling of the TM mode in the dielectric lined slow-wave waveguide to the beam mode via the electron beam. And the coupling is proportional to the density of the beam. The growth rate of the wave produced by the electron beam are obtained. Then, the case of a relativistic electron beam guided by a longitudinal magnetic field in the same slow-wave structure is examined. The motion of electrons could be approximated to be one-dimensional when the simultaneous condition of the beam-wave interaction of dielectric Cherenkov maser is satisfied. Finally, the effect of the background plasma on the instability of the beam-wave interaction is studied.     

用磁化电子束提高自由电子激光器的增益

正 自由电子激光器有可能产生从毫米波到可见光范围内的相干辐射,实现简单的电压连续调谐并能获得极高的输出功率。因此越来越引起人们的重视。它的工作机理可概述如下:当相对论电子束与入射的泵浦电磁波相互作用时,在电子束中激起纵向密度波并产生正向及反向的散射电磁波。我们仅考虑反向散射波,因为它经过两次多普勒频     

等离子体圆柱波导慢电磁波的激励

本文在考虑等离子体厚度效应的情况上,详尽地推导了充填圆环状等离子体的圓柱波导中TM模慢电磁波的色散方程;利用相对论空间电荷波理论,导出了相对论电子注在轴向磁场引导下沿等离子体内表面传输时的空间电荷波方程;求得了电子注和慢空间电荷波相互作用的线性增益和频率漂移;讨论了等离子体厚度、密度对色散特性和互作用增益的影响。     

Magneticresonant three dimensional kinetic theory of the free electron laser with waveguide cavity

Vlasov kinetic theory of the free electron laser employing waveguide frifting tube and helical pump is presented. Distinct from the former theories this theory has (1) taken into account the 3-d structure of the scattering field; (2) applied the plasma kinetic theory, which is more accurate than the other methods, to analysing the effect of the longitudinal. field; (3) taken account of the influence of the annular structure of the beam. The magnetic resonant effect appearing when the cyclotron frequency of electrons approaches the effective frequency of the magnetic pump is analysed and the growth rate formula in the linear regime derived. Results show that on taking into account the 3-d structure of the field and beam, one cannot arbitrarily choose the radius of the hollow beam, or else within certain range the instability may disappear altogether. Lastly, the equation for determination of the optimum beam radius is given and the possibility of raising growth rate by operating in high order modes shown.     

Theory of a nonwiggler collective free electron laser in uniform magnetic field

A nonwiggler free electron laser, operating in uniform guide magnetic field, is analyzed. The amplifier problem is solved self-consistently on the basis of the kinetic theory. It is shown that the asymmetry in the azimuthal distribution of the electrons' momentum leads to a coupling between the transverse and the space-charge modes. This, in turn, enhances the gain in the amplifier. In the case of a cold beam, with the electrons gyrating coherently, the spatial growth in the collective nonwiggler free electron laser (FEL) is comparable to that found in conventional free electron lasers operating in similar regimes.     

自由电子激光中自发辐射光脉冲的自干涉现象

本文用格林函数法,计算了螺旋磁场自由电子激光中单脉冲电子注的自发辐射;结果表明,电子注的有限长度会引起自发辐射光脉冲的自干涉现象。     

Optimization of the beam configuration in the Raman-type free-electron laser

A theoretical discussion is given for the two-dimensional Raman-type free-electron laser composed of a hollow relativistic electron beam of arbitrary thickness contained in a parallel plate waveguide and an array of permanent magnets for the pumping source. Under the influence of the magnetostatic field pump, the coupling between the scattered wave of the even TE mode (positive-energy wave) and the electron plasma wave of the odd TM mode (negative-energy wave) is investigated in detail. With the aid of numerical illustrations, the electron plasma wave with odd symmetry is found to be split into two modes: one mode is dominant for a thick beam and the other mode dominant for a thin beam. For the case where the scattered wave interacts with the electron plasma wave of the latter mode, an optimum beam thickness is obtained for which the growth rate becomes maximum. The optimum beam thickness is found to be comparable with the wavelength of the scattered wave and yet considerably greater than the reactive skin depth of the electron beam. In addition, the efficiency for energy conversion is found to be greatly improved by utilizing a hollow beam instead of a solid beam.