超短脉冲光束传输的时间分辨功率谱

利用小波变换（WT）对超短高斯脉冲光束作时频分析，获得了光脉冲的时间分辨功率谱，给出了在1个脉冲周期内频随时间变化的关系。对光脉冲在自由空间传输的时频谱特性进行了研究，结果表明：在离轴点上，时频谱相对光束中心出现明显的时间延迟，而频谱分布不变。     

光纤光栅中反射带隙附近的强高斯光脉冲的类孤立波特性

利用变分原理 ,研究了在考虑非线性时 ,频率在反射带隙附近的强高斯光脉冲在光纤光栅中的传输特性。计算表明 ,在假设其高斯形状保持不变的一级近似下 ,光脉冲的脉宽和振幅都不发生变化 (即类似于孤立波特性 ) ,而同时在脉冲中会产生一个随传输距离而变的线性啁啾。     

单周期超短脉冲光束通过色散介质的传输

本文分析了单周期超短脉冲光束在色散介质中的传输特性，给出了相应的解析解。结果当脉冲宽度短至几个光学周期时，时空参量之间的耦全变得很重要，并将引起脉冲光束的非对称。     

超短啁啾高斯脉冲叠加光束的空间异常特性分析

以ICF系统应用为背景，建立了四束超短啁啾高斯脉冲远场能量叠加分析模型，分别对单束及多束超短啁啾高斯脉冲的空间异常特性进行了数值模拟和分析。结果表明:脉宽是影响超短啁啾高斯脉冲叠加光束产生空间异常现象的主要因素。在利用指数函数复振幅包络的解析式进行分析时，使用脉宽小于1个光振荡周期的超短啁啾高斯脉冲进行叠加应控制参数在合理的范围内，r1w0时可有效避免空间异常现象。     

部分相干脉冲光束的M2因子

研究了部分相干超短脉冲光束的M2因子。从时空维格纳分布函数出发,以高斯-谢尔(GSM)脉冲光束为例,导出部分相干超短脉冲光束的M2因子公式。给出了空间完全相干高斯脉冲光束和准单色高斯-谢尔脉冲光束的M2因子。由于受脉冲光束带宽及空间相关度的影响,高斯-谢尔脉冲光束的M2因子总是大于1。研究结果表明,M2因子随脉冲光束带宽的增大而增大,随空间相关度的增大而减小。此外,对于啁啾高斯-谢尔脉冲光束,M2因子还随啁啾参数的增大而增大。     

Changes of super-Gausian beams upon propagation

为说明超高斯光束的传输特性，以及光强（振幅）分布的位相的变化，进行了大量数值计算。还研究了超高斯光束通过近轴光学系统时，保持其形状和阶数不变的条件。     

双曲正弦平方-高斯光束在单轴晶体中垂直于光轴的传输

基于光束在单轴晶体中的傍轴矢量传输理论,对双曲正弦平方-高斯光束在单轴各向异性晶体中垂直于光轴的传输做了研究,得到了一般的解析传输公式,并用数值计算方法分析了该光束的传输特性。研究表明:由于晶体的各向异性,其原来的偏振特性将不再保持,仅沿x方向偏振的初始场分量衍生出y分量;随着传输距离的增加,非寻常光沿x轴和z轴的偏振场慢变振幅均减小,光强峰值也随之减小。此外,双曲正弦平方-高斯光束在单轴晶体中垂直于光轴传输时,光束参数β取值不同,光强呈现不同的分布状态。     

圆形平顶高斯光束阵列在湍流大气传输中的M2因子

应用Wigner分布函数的二阶矩定义和拓展Huygens–Fresnel原理研究了圆形平顶高斯光束阵列在湍流大气传输中的光束性质,得到其传输质量因子（ 因子）的解析表达式,进行了相应的数值计算和模拟。结果表明：在湍流大气中传输时,圆形平顶高斯光束阵列的传输质量因子随传播距离、湍流大气结构常数的增大和束腰宽度的减小而增大;当光束阵列阶数一定,阵列个数不断增加时,其传输质量因子先保持不变,然后开始减小,最后不再减小,而保持这个定值不变;当光束阵列的个数一定,阶数不断增加时,其传输质量因子减小,最后不再减小而保持不变。在自由空间中传输时,圆形平顶高斯光束阵列的传输质量因子保持不变。     

超短脉冲高斯光束经聚焦透镜的光场形式

考虑到激光腔模中光腰的频率依赖性 ,得到了超短脉冲高斯光束经消色差透镜聚焦后光场的解析形式 ,并讨论了此时透镜群速度色散对光束聚焦性质的影响。分析了单透镜色差和群速度色散对超短脉冲高斯光束聚焦的时间分布及脉冲波面的影响 ;比较了消色差透镜及单透镜中脉冲初始光腰尺寸对聚焦的影响。     

超高斯光束传输中的变化

为说明超高斯光束的传输特性,以及光强(振幅)分布的位相的变化,进行了大量数值计算。还研究了超高斯光束通过近轴光学系统时,保持其形状和阶数不变的条件。     

阵列辐射瞬态电磁脉冲能量合成特性研究

根据单元天线辐射瞬态电磁脉冲轴线能量传输特性的解析解,提出了阵列辐射瞬态电磁脉冲的点源近似模型,给出阵列辐射瞬态电磁脉冲高效合成特性的物理实质。并采用阵列瞬态电磁脉冲产生系统,对高效合成特性进行实验验证。实验结果和采用点源近似模型计算结果都很好地证明了阵列瞬态电磁脉冲的高效合成特性。     

Sommerfeld Pre- and Postcursors in the Context of Waveguide Transients

For propagation in lossless waveguide, the rigorous impulse response function is given. It is shown that its instantaneous frequency is that which has reached the output at that time by propagating at the group velocity. For a square envelope pulse with a carrier frequency /spl omega/ above the cutoff frequency /spl omega//sub c/, the propagation of the envelope and of the phase are essentially described by the group and phase velocity, respectively. In addition, however, the bulk of the pulse is preceded by the so-called Sommerfeld precursors having an increasing amplitude and a frequency which decreases from a high value to /spl omega/. Similarly the bulk of the pulse k followed by the Sommerfeld postcursors in which both amplitude and frequency decrease, the latter from /spl omega/ to /spl omega//sub c/. The analytic results are illustrated by computed examples of waveguide transients.     

A complex radio signal in ionospheric plasma

Analytic solution of the problem on propagation of a frequency-modulated radio pulse in cold isotropic collisional plasma is presented. The solution does not involve the Fourier integral and is not restricted to the distance of propagation or to the a priori choice of the shape of the initial pulse envelope. Rectangle pulses with linear and V-shaped frequency modulation and a trapezoidal pulse with linear frequency modulation are considered. The obtained solution is applied to analysis of distortions of such pulses during propagation along an ionospheric path. It is shown that the solution is efficient in the analysis of the uncertainty function of a propagating pulse     

Response of Quasi-Peak Detector to Periodic Impulses with Random Amplitudes

The known result for the output reading of a quasi-peak detector to periodic pulse inputs is here extended to cover inputs made up of regularly repeated pulses of the same shape, but with random amplitudes. The cosine envelope was chosen for the pulse shape and is viewed as a satisfactory approximation for the typical IF amplifier impulse response. The probability distribution for the pulse amplitude was assumed uniform over an amplitude interval; the latter is a parameter in the analysis so that the result applies, at one extreme, to pulses ranging randomly from zero amplitude to some maximum, and at the other extreme, to fixed amplitude pulses. Solutions are provided for low-frequency inputs-such as would be developed at the output of an IF amplifier followed by an envelope detector, and RF inputs-such as would be found directly at the IF amplifier output.     

Exact solution of a π-pulse problem

The exact solution describing steady-state resonant pulse propagation in a two-level inverted medium is given. This steady-state pulse is often referred to as a 180° or π-pulse. No approximation of a slowly varying envelope is made, and hence the solution satisfies the second-order wave equation as well as the equations of motion of the density matrix of the system. As a result the theory is able to describe very short pulses, whose width can be of the order of the period of the optical carrier. The model for the system includes a nonresonant loss and a finite value of the transverse relaxation time T2, but neglects dispersion in the host medium. The steady-state pulse is found to be frequency modulated and asymmetric in shape.     

分析任意光脉冲传输的矩阵方法

本文用矩阵分析方法讨论了任意时间场分布的光脉冲在一般色散介质中的传输,引入了光脉冲质量因子M_τ~2和一般化的脉冲复参数P~(-1),得到了具有任意形状和任意啁啾的光脉冲在色散光学系统中传输的ABCD定律。     

Propagation of intense microwave pulses in air and in a waveguide

The state of research on intense electromagnetic pulse propagation in air and in waveguides is reviewed. Some results obtained from recent investigations of the propagation of intense electromagnetic pulses in the atmosphere and in an air-filled waveguide when the field strength is above the threshold for air breakdown are presented. It is shown how the air breakdown affects the shape of the pulse. In addition, the accuracy of the calculational models is discussed, comparing calculations with experimental data     

Electromagnetic pulse propagation in a weakly nonlinear plasma

An investigation of the propagation of electromagnetic pulses in a weakly nonlinear, cold, collisionless plasma is described. It is found that a transverse electromagnetic pulse generates, through nonlinear effects, a small amplitude, longitudinal electric pulse field. The transient behavior of this longitudinal electric field is studied. One particular case is considered in detail: the nonlinear generation of a longitudinal electric field by a transverse electromagnetic pulse which is excited by a suddenly turned-on cosinusoidal electric field of frequencyomega_{0}. Computer plots of numerical calculations of the second-order transient longitudinal field are presented.     

三阶色散对光纤中基孤子脉冲传输的影响

通过数值求解非线性薛定谔方程,研究了三阶色散效应对基孤子脉冲在单模光纤中传输的影响.结果表明,在三阶色散作用下,基孤子脉冲在传输过程中被展宽,峰值能量逐渐减小,脉冲形状发生畸变,脉冲的中心偏向一侧,并形成非对称的拖尾振荡结构;当与二阶色散共同作用时,三阶色散引起的脉冲振荡会变缓.考虑非线性效应后,在一定程度上补偿了由于色散效应导致的峰值功率的减小,同时抑制了非对称拖尾结构的产生.     

Lateral electromagnetic waves and pulses on open microstrip

The propagation of lateral electromagnetic waves and pulses on microstrip is investigated. Interference patterns generated by the superposition of the lateral and direct waves along the air-substrate surface are shown. The field generated by the pulse excitation of a horizontal dipole on the air-substrate boundary is shown to consist of a lateral-wave pulse and a slower direct-wave pulse. Their differences in shape and decay rate are clarified. It is shown that the shape of a Gaussian pulse propagating along an open microstrip transmission line is closely related to the shape of the lateral electric-field pulse generated by a Gaussian current pulse in a dipole on the air-substrate boundary