基于Hilbert变换的LFM检测与估计

LFM(线性调频)信号是一类重要的非平稳信号,其完全被初始频率和调频斜率两个参量表征,而LFM信号的检测与估计问题是信号处理中最为重要的研究热点之一.由于调频信号在时频平面内有较好的聚集性,通常使用时频分析的方法对其进行检测和估计.线性正则变换是经典时频分布的广义形式,对LFM信号具有很好的能量聚集特性,在现有的线性正则域Hilbert变换的基础上,提出了一种不需要谱峰搜索而快速检测LFM信号和估计其参数的方法,并且通过仿真实例验证了所提出方法的优越性.     

基于MgO:APLN的1.57μm/3.84μm连续波内腔多光参量振荡器研究

报道了一种基于MgO:APLN实现1.57 μm和3.84 μm跨周期参量光连续输出的内腔抽运多光参量振荡器. 采用1064 nm谐振腔与多光参量振荡腔折叠型复合结构, 综合考虑高功率抽运下谐振腔的热稳定性及多光参量振荡过程的光斑模式匹配, 通过对两个子腔谐振结构的数值模拟分析, 确定了最佳腔型参数. 在此基础上, 进一步研究了谐振参量光透过率对振荡阈值、抽运光下转换效率、输出功率稳定性的影响, 最终实现了3.13 W的1.57 μm和0.85 W的3.84 μm参量光输出, 对应斜效率为6.8%和1.9%, 输出功率稳定性分别达到了1.8%和3%.     

连续波氧碘激光对光伏型锑化铟探测器的破坏阈值

 通过测量光伏型锑化铟探测器在不同功率密度的连续波氧碘激光辐照下性能的变化,得到其破坏阈值范围为26(089s)～113(14s)W/cm²。 理论上用一维热模型计算了探测器在激光辐照过程中温升和输出信号的变化过程,对实验结果进行了分析。     

10kW连续波固体推进剂燃烧驱动CO2气动激光实验研究

 简要介绍了固体推进剂燃烧驱动连续波CO₂气动激光系统的工作原理及其突出特点，对组成10kW实验系统的各主要部件——固体推进剂燃气发生器、超音速掺混室、喷管 排、谐振腔等作了简要说明,利用该实验系统进行了上百次成功的测量或打靶实验,并对主要实验结果进行了总结分析。     

单模石英光纤中连续波泵浦SRS谱的演化

利用连续波掺Yb双包层光纤激光器为泵浦源,对单模石英光纤中受激Raman散射谱的形成过程进行了实验研究结果表明,由自发Raman散射向受激Raman散射演化的过程中Stokes谱宽度不断变窄当Stokes波信号功率较强时,在Raman光谱内部会出现能量红移现象,使Stokes光谱峰值相对于泵浦波的频移量从440cm^-1转化到490cm^-1.     

一种低频大功率调频声波束扫描发射系统

本文介绍一种中心工作频率在４．５ｋＨｚ发射电功率８ｋＷ的１６基元线列阵发射系统，并介绍了使用ＤＳＰ５６００１数字信号处理产生线性调频扫描波束发射信号及接收信号的频域处理和和一些测试结果。     

无线调频基地台的DTMF选呼

介绍了无线调频基地台的ＤＴＭＦ选呼系统的硬件和软件。它用８７５１作主控器，以独特的中断非正常返回构思大大简了编程，并提高了系统的可靠性。     

Effects of modulation amplitude and frequency of frequency-modulated fiber lasers on the threshold of the stimulated Brillouin scattering in optical fiber

Stimulated Brillouin scattering （SBS） is a key problem with the increasing power of fiber transmission systems. In this letter, a frequency-modulated fiber laser with an ultra-narrow linewidth is chosen as a light source. The SBS threshold is increased from 4.1 to 6.2 mW at 13-MHz frequency modulation amplitude for a 50-km G652 fiber. We also show that the SBS threshold increases with not only the frequency modulation amplitude, but also the modulation frequency. The modulation frequency should be high enough for effective modulation.     

FM-AM Conversion Induced by Polarization Mode Dispersion in Fiber Systems

The conversion of the frequency modulated pulse induced from frequency modulation （FM） to amplitude modulation （AM） by the polarization mode dispersion （PMD） is theoretically and experimentally investigated. When there is no polarizer at the output end of a fiber system, the amplitude modulation depth is stable by 8%. Random amplitude modulation is observed when a polarizer is placed at the output end of the fiber system. The observed minimum and maximum modulation depths in our experiment are 5% and 80%, respectively. Simulation results show that the amplitude modulation is stable by 4% induced mainly by group velocity dispersion （GVD） when there is no polarizer, and the amplitude modulation depth displays the random variation character induced by the GVD and PMD. Lastly, a new fiber system scheme is proposed and little amplitude modulation is observed at the top of the output pulse.     

High Power Continuous-Wave Actively Mode-Locked Diode-Pumped Nd:YAG Laser

We demonstrate a diode-pumped cw mode-locked Nd：YAG by an acousto-optic mode locker. A mode-locked pulse with duration of 345 ps and output power of 12 W is obtained. The resonator design shows three advantages： a larger mode volume, high stability against thermal lens fluctuations, and excellent beam quality with TE00 mode. Different from previous active mode locking designs, we employ a frequency stabilizer and a phase-lock loop circuit to ensure the mode locking stable operation.