海面动态波动引起的船舶辐射噪声线谱伴随调制特性

针对海上实验发现的船舶辐射噪声载波线谱两侧对称出现伴随线谱现象,建立了基于抛物方程近似理论的动态起伏海面条件下连续波信号传播预报模型,揭示了海面风速、收发距离、声源深度等因素对伴随调制线谱频率间隔和强度的影响规律。数值仿真结果表明,伴随调制线谱与其载波线谱的频率间隔由具有稳定频率的海面涌浪决定;伴随调制线谱强度随海面风速增大而增大;不同收发距离和声源深度等条件下伴随调制线谱强度随距离的变化趋势与其载波线谱强度基本一致,近水面（平均深度3 m以内）声源上移和下移伴随调制线谱能量大致相当,比载波线谱能量低约10 dB;除了载波传播损失大的深度外,非近水面声源上移和下移伴随调制线谱强度能量相差较大,比载波线谱能量整体上低约20 dB以上。对海上实测水面船辐射噪声数据进行长时间窗时频分析表明,上移和下移频率伴随调制线谱与载波线谱的间隔为0.1 Hz左右,伴随调制线谱强度与载波线谱强度相差约10 dB,与仿真分析结果一致。海面动态波动引起的船舶辐射噪声线谱伴随调制特性对水中目标特征识别等具有重要价值。      

光谱色散匀滑技术与衍射光学器件联用性能的空间频谱分析

基于空间频谱分析方法，建立了光谱色散匀滑技术(SSD: Smoothing by Spectral Dispersion)与衍射光学器件(DOE: Diffractive Optical Element)联用性能的简化分析模型，为SSD与DOE联用时，SSD参量的优化提供了理论依据.数值模拟了SSD各参量，包括脉冲时间、调制频率、位相调制系数、光栅线色散系数等对束匀滑性能的影响.模拟结果表明，SSD参量经过优化选取，且波前畸变随时间快速变化时，能获得良好的束匀滑性能.     

双三角形结构的光纤光栅压力和温度双参量传感器

为解决压力和温度同时测量时的交叉敏感问题,提出一种基于双三角形悬臂梁结构的光纤光栅压力、温度双参量测量传感器. 在外界压力作用下,光纤布喇格光栅反射谱分裂成双峰结构,悬臂梁的应变调制传感光纤光栅双峰间距,温度变化转变成反射谱整体的移动. 实验结果表明该结构可实现单光栅双参量测量,且具有良好的线性和可重复性.     

低串扰的多波长光纤光栅色散补偿器

分析了光纤光栅色散补偿系统中的串扰，并比较了几种常用的多波长光纤光栅色散补偿器的串扰特性，结合串联的窄带光纤光栅和取样光纤光栅的优点，提出一种抑制光纤光栅色散补偿系统串扰的方法.它通过在邻近信道间引入随机时延差，既能改善取样光纤光栅的线性串扰特性，又能抑制交叉相位调制效应和四波混频等非线性串扰.使用该方法可以得到具有低串扰的多波长光纤光栅色散补偿器.     

滑动盖板对一维微尺度光栅红外辐射特性影响

电磁波入射到微尺度周期性结构表面时,一定条件下将在某一波段产生异常光吸收现象。基于该特性,本文提出了单边移动盖板光栅和双边移动盖板光栅两种光栅结构,并使用严格耦合波分析(RCWA)方法对TM波垂直入射的一维微尺度光栅表面辐射特性进行了分析,研究了滑动盖板的厚度和位置对光栅表面结构辐射特性的影响。结果表明,相同盖板厚度,双边移动盖板光栅形成的发射率峰较单边移动盖板光栅形成的发射率峰具有较宽的半高全宽(FWHM),但峰值较低;随盖板向关闭侧移动,高发射率峰对应波长向长波方向移动;随盖板厚度增加,发射率峰向长波方向移动,其中双边移动盖板光栅结构形成的发射率峰变宽,峰值变小。     

双锥型光纤布喇格光栅光谱特性

利用传输矩阵法和有限元法分析了光栅周期、调制深度、锥腰直径和不同设计区段长度比等光栅制作参量和结构设计参量对双锥型光纤布喇格光栅光谱特性的影响.软件仿真结果表明:限定相关参量后,光栅周期增大,双锥型光纤布喇格光栅整体反射谱右移,与均匀分布光纤布喇格光栅光谱变化规律一致;调制深度增强,两主反射峰基本不变,而两主反射峰中间的次级峰个数增多,光强增大;锥腰直径减小,激发更多包层模,干涉峰个数增多,强度提升;整根光栅长度保持1cm不变,锥腰区,标准光栅区和渐变光栅区长度比直接影响次级峰的数量和幅值,随着渐变光栅区长度占比的增大,次级峰的幅值增大,同时个数减少.双锥型光纤布喇格光栅可在多参量传感器、多通道滤波器、多通道半导体激光器、色散补偿和光上下载分插复用等方面广泛应用.     

光纤布拉格光栅γ 辐射损伤及其对光谱特性的影响

基于色心产生模型理论分析了电离辐射对光纤布拉格光栅的影响, 并推导出了光栅有效折射率变化与辐射剂量的函数关系式. 使用⁶⁰Co γ辐射源对光纤布拉格光栅进行了总剂量为1× 10⁶ rad的电离辐射实验, 实验结果与理论符合较好. 在辐射环境下, 光栅反射谱的峰值波长随着剂量增加向着长波方向移动, 由其计算所得的辐射致折射率变化规律与所得到的函数关系式相符. 该公式结合低剂量辐射实验可预测光栅在高剂量辐射下的性能变化, 对评估光栅产品抗辐射特性, 及筛选出性能较好产品有着实际应用价值.     

基于啁啾光纤光栅时分延时的相控阵波束形成

利用脉冲调制雷达信号的间歇性工作特点,不同波长的激光与雷达信号进行时分调制。啁啾光纤光栅将已调制射频信号的一串光脉冲序列进行反射延时,不同波长的激光序列在不同位置反射后产生不同时延。对载波频率等于4GHz的脉冲雷达信号进行实验测量,结果表明4个阵元的延时值与波束指向的理论延迟值一致,满足系统设计要求。     

湿端结构极简的低噪声低串扰光纤光栅水听器阵列

由于湿端极简化,光纤光栅水听器系统中普遍存在的偏振诱导信号衰落和随机相位衰落等关键问题仅能采用复合型调制解调手段解决;光纤光栅的双向反射特性会引起传感通道间信号串扰增加等新问题。报道了一种光纤光栅水听器阵列,水下仅采用80个光纤光栅构成64基元水听器阵列。采用相位生成载波与偏振切换调制解调方案,系统本底相位噪声达到■,等效噪声压为36 dB@1 kHz。系统采用低反射率光纤光栅,结合8空分×2波分×8时分复用结构设计,系统的时分、空分和波分通道串扰均稳定在-40 dB以下。该研究为光纤光栅水听器的工程实用化提供了重要的实践探索。     

聚合物费米型截面阵列波导光栅的优化设计

利用微扰理论给出“等效矩形波导法”,分析了费米型截面硅基聚合物阵列波导光栅的传输特性.模拟表明,波导的费米型截面将使阵列波导光栅的传输光谱产生漂移、并使串扰增大.为了消除光谱漂移、减小串扰、实现正常的解复用功能,对阵列波导光栅的结构参量进行了重新优化.结果表明,重新设计的费米型截面聚合物阵列波导光栅的光谱响应和串扰恢复到初始设计的聚合物矩形截面阵列波导光栅的水平.     

Observation of frequency-locked coherent terahertz Smith-Purcell radiation

We report the observation of enhanced coherent Smith-Purcell radiation (SPR) at terahertz (THz) frequencies from a train of picosecond bunches of 15 MeV electrons passing above a grating. SPR is more intense than other sources, such as transition radiation, by a factor of Ng, the number of grating periods. For electron bunches that are short compared with the radiation wavelength, coherent emission occurs, enhanced by a factor of Ne, the number of electrons in the bunch. The electron beam consists of a train of Nb bunches, giving an energy density spectrum restricted to harmonics of the 17 GHz bunch train frequency, with an increased energy density at these frequencies by a factor of Nb. We report the first observation of SPR displaying all three of these enhancements, NgNeNb. This powerful SPR THz radiation can be detected with a high signal to noise ratio by a heterodyne receiver.     

介质层充电对光栅光调制器驱动的影响

利用高斯定理分析了二氧化硅层中存在电荷时,光栅光调制器中的空间电场分布,得到了光栅光调制器在介质层存贮电荷影响下的静电力公式. 分析了调制器中二氧化硅介质的充电和放电机理,得到了光栅的位移随介质充放电的变化关系. 通过分析指出当驱动电压的周期和介质的充放电时间常数相近的时候,介质层中存贮的电荷会使得可动光栅被下拉后发生缓慢的回跳. 电压被撤消后,光栅会受到存贮电荷所产生电场的作用而被下拉. 当驱动电压的周期远小于介质的充放电时间常数的时候,随着存贮电荷的增加,光栅在有外加电场时被下拉的距离和外加电场为零时被下拉的距离逐渐相等,光调制器输出光的光强变化逐渐减弱,当存贮电荷产生的电场为外加电场的一半时,器件完全失效. 通过实验对理论分析的结果进行了验证,实验结果和理论分析一致. 文章最后提出了一种消除介质层所存贮的电荷的方法,通过实验证明了这种方法的可行性. 关键词： 微机电系统 光栅光调制器 介质层充电     

Quasi-stellar objects as Čerenkov sources

If a beam of ultrarelativistic charges enters a gas cloud ?erenkov radiation may be produced. The condition for such radiation is given, and the ?erenkov power radiated per charge is compared to the synchrotron power. Intense ?erenkov pulses will excite emission lines via stimulated Raman scattering. Due to anomalous dispersion in the presence of ac Stark effect the ?erenkov field will be most intense at frequencies well red-shifted from atomic resonances, and this red-shift will be a feature of the stimulated Raman line emissions. The intensity ratios and anomalous red-shifts of the broad emission lines of QSOs can be explained. ?erenkov emission froma collimated beam will be highly directional. The emission evidently does not occur in BL Lacs, which are pure synchrotron emitters.     

Characteristics of terahertz coherent transition radiation generated from picosecond ultrashort electron bunches

This paper presents a method of generating terahertz (THz) coherent transition radiation (CTR) from picosecond ultrashort electron bunches including single and train bunches, which are produced by a photocathode radio frequency gun. The radiation characteristics of THz CTR including formation factor and energy spectrum are analysed in detail. With the help of a 2-dimensional particle-in-cell simulation, the radiation characteristics including power, energy and magnetic field are analysed. The results show that the radiation frequency can be adjusted by tuning the repetition frequency of the train bunch and the energy can be enhanced with the train bunches.     

Simultaneous temperature and refractive index measurement of liquid using a local micro-structured fiber Bragg grating

An alternative solution for the simultaneous measurement of temperature and refractive index is presented. A local micro-structured fiber Bragg grating（LMSFBG）is formed as the sensing head,in which a standard grating is etched by HF.According to the phase shift theory,the main spectral change of the LMSFBG is the formation of a narrow allowed band,which is strongly dependent on the etching features and the surrounding refractive index.As such,the temperature and refractive index measurements can be achieved by the shifts of the double peaks and narrow allowed band,and their fitting linearity coefficients are 0.996 and 0.994,respectively.Thus,the reflection and transmission peaks of the LMSFBG have a good linear relationship with temperature and refractive index.     

Widely tunable monolithic narrowband grating filter for near-infrared radiation

We propose a monolithic narrowband guided-mode grating filter in fused silica that is widely tunable in the near-IR wavelength region. Based on a recently demonstrated approach for a monolithic reflector comprising an encapsulated grating, we theoretically investigate such a device by means of rigorous modeling aimed at a narrow linewidth. It is demonstrated that upon a spatial variation of the filter's grating period its resonance wavelength can be tuned in a remarkably wide range of near-IR radiation with 800 nm<λ(res)< 1600 nm by translating the laser beam relative to the grating area. The filter performance in terms of linewidth and contrast is essentially preserved over the entire tuning interval.     

Characteristics of the formation of an electromagnetic wave field with an instantaneous change in the states of charges

It is shown that in the process of annihilation and neutralization of two moving charges of opposite sign, energy is not radiated at the instant of the disappearance of the charges, but is formed later from the energy of the magnetic fields of the disappearing charges, i.e., a reaction effect occurs. An analogous effect will also occur in other radiation processes such as the instantaneous starting and stopping of charges, their instantaneous creation and the electrification of bodies, etc. The existence of the reaction effect in the radiation of electromagnetic energy by charges seems to be an essential defect in macroscopic electrodynamics.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 11, pp. 93–95, November, 1982.     

Ionisation of Rydberg hydrogen atom near a metal surface by short pulse laser

In the ionisation of Rydberg hydrogen atoms near a metal surface,the electron will escape from the nucleus and arrive at the detector in a time sequence.This probability flux train relies on the initial electron wave packet irradiated by the laser pulse.For simplicity,the laser pulse is usually simplified to a delta function in energy domain,resulting in a sharp initial arrival time with an exponentially decaying tail at the detector.Actually and semiclassically,the initial outgoing wave should be modeled as an ensemble of trajectories propagating away from the atomic core in all directions with a range of launch times and a range of energies.In this case,each pulse in the pulse train is averaged out rather than a sharp profile.We examine how energy and time averaging of the electron wave packet affects the resolution of escaping electron pulses and study the energy dependence of the arrival time for each pulse in the ionisation train.An optimization condition for the laser pulse shape to generate narrow ionisation electron pulse in the train is obtained.The ionisation rates with various excitation energy are calculated also,which show the excitation to higher N Rydberg states will narrow the electron pulse as well.     

Double quasi phase matching for both optical parametric oscillator and difference frequency generation

We present simultaneous phase matching of optical parametric oscillator (OPO) and difference frequency generation (DFG), using a noncollinear interaction in periodically poled crystal with single grating. Selecting proper grating period Λ and titled angle ξ between the grating vector G and the optical axis of crystal, the noncollinear scheme provides double phase matching solutions over continuous regions of the midwave infrared spectrum. At certain wavelength regions, for DFG process the group velocities between interaction pulses are matching and the phase matching bandwidth reaches maximum. Selecting the different grating period, the broadband midwave tuning and better gain spectrum can be obtained at different wavelength range. For the certain period grating the conversion efficiency is higher. Hence, using the double phase matching configuration, the broadband tunable midwave infrared wave can be produced in single grating. But the configurations have a relatively narrow angular bandwidth.