非同步的多普勒水声跟踪定位原理

提出了一种新的水声跟踪定位方法,它仅测量目标非同步声信标到达各测量基元的接收信号和频率,来对目标声学跟踪定位,称之为非同步多普勒定位方法,本文介绍其原理,处和仿真结果。     

复频聚焦超声换能器水中焦区商场特性的研究

本文对新研制的一种复频聚焦超声换能器的辐射声场进行了实验研究,测定了辐射压在轴向上的分布曲线,进而确定了焦区位置,这与理论所得结果符合较好,测定了辐射声压在焦平面上的分布曲线,并对焦区声场进行了定位,最后对换能器在水中焦区辐射声的频谱进行了研究,不仅观测到了两个源波,而且还观测到了和频波,差频波以及倍频波,证实了声散射声效应的存在。     

基于AR模型的人体脉象信号模糊聚类研究

根据一种新的模糊聚类方法－F－PFSR（Fuzzy Pseudo F-Statistic Ratio)聚类法,对人体脉搏声信号（脉象信号）进行了聚类识别研究。首先对脉搏声信号作8阶AR模型拟合,模型系数构成信号的特征集,其次采用K－L变换对特征集进行了压缩,最后对临床实测脉象信号进行了聚类分析。实验结果表明,本文的聚类方法是可行和有效的。     

超声波作用下声学参数对悬浮液中微粒凝聚的影响

对利用超声波去除或分离悬液中微小颗粒过程中频率和时均声能密度等声学参数对微粒凝聚的影响作了分析研究。利用前人的数学模型对不同声对比因数下悬浮液中微粒达到平衡状态时所需要的时间及凝聚位置进行了计算。在水模型实验,实验中所施加超声波的频率为24.1kHz,微粒的粒径为0-60um、密度940kg/m^3的高密度聚乙烯,实验液为脱气软化水,实验结果与部分理论分析结果是一致的。     

超短脉冲光束传输缓变包络近似理论的失效和空间奇异性的形成与消除

研究了单周期或更短的超短脉冲光束在真空中的传输.结果显示,在此情况下缓变包络近似理论已不再有效,其失效的原因是,该理论导致了脉冲光束解的空间奇异性,并使脉冲光束不再具有符合物理意义的光束行为,而通过复解析信号的分析方法可以消除这种空间奇异性.给出了时间波形为Gauss,Hyperbolic Secant和Lorentz的脉冲光束奇异性的计算模拟,并给出了解决这些奇异性的复解析信号解.同样,会发现在脉冲光束超过一定的长度后两种解是一致的.     

干涉条纹场成像的目标重建

分析环状条纹干涉成像的信号提取方式,用计算机模拟目标二维图像的重建方式,研究干涉环中心在照明场中心的位置对点扩展函数的影响,并用实验论证上述影响。     

二阶级联声光双稳态超浑沌的周期驱动控制

本文提出了对二阶级联声光双稳态超浑沌进行外周期激励,从而实现了对其进行有效控制.     

磁场对光轴运信号的影响

摘 要;在做光泵磁共振实验时,分别研究了竖直线圈和水平线圈产生的磁场对光抽运信号的影响．并做出了它们之间的关系曲线．由此曲线计算了北京地磁场的垂直分量为（0. 0881±0·0015）×10-4T ,估算出北京地磁场的水平分量约为 0．425 ×10-4T．同时,这项工作对于区分光抽运信号和磁共振吸收信号也有一定的帮助．     

Influence of Signal and Noise on Statistical Fluctuation of Single-Mode Laser System

On the basis of calculating the steady-state mean normalized intensity fluctuation of a signal-mode laser system driven by both colored pump noise with signal modulation and the quantum noise with cross-correlation between its real and imaginary parts, we analyze the influence of modulation signal, noise, and its correlation form on the statistical fluctuation of the laser system. We have found that when the amplitude of modulation signal weakens and its frequency quickens, the statistical fluctuation will reduce rapidly. The by reducing the intensity of pump noise and quantum noise. statistical fluctuation of the laser system can be restrained Moreover, with prolonging of colored cross-correlation time, the statistical fluctuation of laser system experiences a repeated changing process, that is, from decreasing to augmenting, then to decreasing, and finally to augmenting again. With the decreasing of the value of cross-correlation coe~cient, the statistical fluctuation will decrease too. When the cross-correlation form between the real part and imaginary part of quantum noise is zero correlation, the statistical fluctuation of laser system has a minimum. Compared with the influence of intensity of pump noise, the influence of intensity of quantum noise on the statistical fluctuation is smaller.     

The statistical fluctuation of a single-mode laser system driven by coloured pump noise with signal modulation and the quantum noise with cross-correlation between its real and imaginary parts

Using the linear approximation method, this paper studies the statistical property of a single-mode laser driven by both coloured pump noise with signal modulation and the quantum noise with cross-correlation between its real and imaginary parts, and calculates the steady-state mean normalized intensity fluctuation and intensity correlation time. It analyses the influences of the modulation signal, the net gain coefficient, the noise and its correlation form on the statistical fluctuation of the laser system respectively. It is found that the coloured pump noise modulated by the signal has a great suppressing action on the statistical fluctuation of the laser system; the pump noise self-correlation time and the specific frequency of modulation signal have the result that the statistical fluctuation tends to zero. Furthermore, the `colour' correlation of pump noise has much influences on the statistical fluctuation of the laser system. Increasing the intensity of pump noise will augment the statistical fluctuation of the laser system, but the intensity of quantum noise and the coefficient of cross-correlation between its real and imaginary parts have less influence on the statistical fluctuation of the laser system. Therefore, from the conclusions of this paper the statistical property can be known and a theoretical basis for steady operation and output of the laser system can be provided.