气泡浓度对海洋激光雷达后向散射特性的影响

对不同浓度气泡幕水下激光雷达的后向散射特性进行了理论分析和实验研究。实验结果表明：由于水中气泡群后向散射的原因,在水下激光雷达整体后向散射信号的回波曲线上,除了水体后向散射导致的信号峰以外,还出现因气泡散射而导致的散射峰,该散射峰叠加在水体的后向散射信号峰上,其位置与水中气泡幕的位置直接相关,而其幅值则受气泡幕的浓度影响。随着气泡幕浓度的增大,其后向散射峰幅值相应增大,这一点与理论分析结果一致,而回波峰值的变化趋势则主要受水体质量的影响。     

在单模光纤中放大的反斯托克斯拉曼背向自发散射的温度效应

在单模光纤中,输入的激光功率大于阈值时．出现放大的反斯托克斯拉曼背向自发散射现象。实验发现：放大的反斯托克斯拉曼背向自发散射具有温度效应．与反斯托克斯拉曼背向自发散射一样,放大的拉曼散射光的光子通量受到光纤温度的调制。反斯托克斯拉曼背向白发散射的放大效应抑制了单模光纤中的相干噪声,改善了系统的信噪比。实验还发现．放大的反斯托克斯扎曼背向自发散射空域曲线上放大的端点位置随激发功率的增高前移并具有一定的规律性。放大的反斯托克斯拉曼背向自发散射的温度效应作为一种新的测温原理,已应用于远程30km分布光纤温度传感器系统。     

神光Ⅲ原型全孔径背向散射测量系统研制及应用

为了测量激光与等离子体相互作用产生的散射光份额,获得黑腔耦合效率实验中的激光注入率,研制了基于神光Ⅲ原型装置的全孔径背向散射测量系统。该系统利用聚焦透镜收集散射光,通过离轴抛物面镜进行缩束,并采用二向色镜将散射光分为两个支路后分别进行受激布里渊散射和受激拉曼散射光的能量、时间过程和光谱测量。实验测量了有、无束匀滑条件下的散射光份额。结果表明,在当前实验条件下,通过束匀滑可有效降低散射光份额,提高激光注入率。     

Online ef fective backscattering estimation for ring laser gyro

Lock-in phenomenon in ring laser gyroscopes is directly related to effective backscattering,which includes both backscattering and nonuniform loss.Effective backscattering often differs in different states and can only be reflected in a working state via online estimation in the working state.Moreover,effective backscattering can result in the intensity modulation of beams in the opposite directions.The effective backscattering parameters can be obtained by measuring the weak modulations in the intensity signals under different rotation rates and by using the curve-fitting method.This letter demonstrates the online estimation of backscattering.     

浅海小掠射角的海底界面声反向散射模型的简化

在浅海,尤其是负梯度声速剖面和海面较为平静的浅海波导,海底界面反向散射是浅海混响的主要来源.经验散射模型只适用于分析浅海混响平均强度衰减特性,而基于物理机理建立的反向散射模型克服了这一缺陷,但同时也引入了其受地声模型约束的问题.本文结合了海底反射系数的三参数模型,对浅海远场海底反向散射模型进行了简化,以减少地声模型的输入参数.理论分析了海底反射系数的相移参数可以描述海底对声场的散射作用,无需任何海底地声参数的先验知识.通过对海底反向散射模型近似简化,结果表明在临界角附近和甚小掠射角范围内的海底粗糙界面反向散射模型的角度特性和强度特性受海底沉积层的影响不同:在临界角附近,海底反向散射的角度特性受海底反射系数的相移参数加权,而其散射系数则近似与相移参数无关;对于甚小掠射角,海底反向散射的角度特性近似与海底反射系数的相移参数无关,其散射系数则近似与相移参数的4次方成正比.     

水中石油类含量对后向散射系数光谱的影响

根据2008年5月和2009年8月在辽宁省盘锦市石油类污染水体配比试验和现场试验获取的光学特性数据及生物化学特性数据,分析了石油类含量和后向散射系数数据的关系.结果表明:河口区的后向散射系数幂律指数遵循随着悬浮物浓度增加而减小的对数变化规律;440～856 nm波长范围内单位后向散射系数在0.006～0.035 m2g-1之间,并且随波长增加而减小;石油类含量对后向散射系数的影响集中反映在石油类单位后向散射系数(单佗石油类含量的后向散射系数)上,石油类单位后向散射系数与石油类含量呈乘幂变化规律,且随波长的增加而减小;石油类含量对后向散射系数幂律指数影响小.     

佛克脱线型HeⅠ 1 083.0 nm的有效后向散射截面的理论研究

考虑到碰撞展宽导致的洛伦兹线型,理论上研究了佛克脱线型(高斯线型和洛伦兹线型的卷积)HeⅠ 1 083.0 nm辐射线的后向散射截面和有效后向散射截面,HeⅠ 1 083.0 nm辐射线实际上由三条非常接近的1 083.034,1 083.025和1 082.908 nm辐射线组成,文章给出了此3条辐射线的有效后向散射截面的曲线及其峰值,得到的10-16数量级与预言的数量级相一致。此研究比以前假定HeⅠ 1 083.0 nm辐射线为高斯线型更接近实际,从而为共振雷达探测热成层亚稳态He提供了更全面翔实的理论基础。文章还给出了HeⅠ 388.9 nm和HeI 318.8 nm辐射线的有效后向散射截面的曲线及其峰值,得到它们的有效后向散射截面比HeI 1 083.0 nm辐射线的小,此结论与实验结果相一致。     

利用转动拉曼测量大气气溶胶后项散射比

利用大气的弹性散射信号与整个转动拉曼信号的比值,不需要假设任何的气溶胶的消光与后项散射比值,就可得到大气气溶胶的后项散射比。通常测量部分转动拉曼谱线之和代替全部转动拉曼谱线之和。全部的转动拉曼谱线之和是不依赖温度,但部分的转动拉曼谱线之和却是与温度有关的。因此,利用转动部分拉曼谱线之和反演大气气溶胶的后项散射比就会带来误差。模拟了随温度变化不同转动量子数的拉曼谱线之和,并且计算了由这些不同转动拉曼谱线之和反演大气气溶胶后项散射比的误差。然后文章提出了一种新的方法,不需要测量整个转动拉曼谱线之和,而只需要测量单条转动拉曼谱线及大气温度,就可以获得大气气溶胶的后项散射比。最后通过实验给出了实际测量的大气气溶胶的后项散射比的结果。     

1.30-2.21MeV质子在硅上的160°散射截面测量

采用薄靶对能量 1.30 - 2 .2 1MeV质子在纯度为 99.99%硅上的非卢瑟福弹性背散射截面(16 0°背散射角 )进行了测量 .质子束由 2× 1.7MV串列加速器提供 ,测量仪器采用金硅面垒探测能谱仪 .实验中最低能区进入卢瑟福弹性散射能区 ,测量结果与以前发表的结果进行了比较 .所测量数据可供从事背散射分析技术的有关人员参考 . The elastic backscattering cross sections of H + from silicon for a wide energy range are very useful parameters in the proton backscattering analysis for investigating silicon content and distribution profiles in the films. It is necessary to measure the scattering cross sections with good accuracy at a large scattering angle for the applications of proton backscattering analysis. The present paper reports our measured results of differential elastic backscattering cross sections of 1.30-2.21 MeV...     

Backscattering enhancements from Rayleigh waves on the flat face of a tilted solid cylinder in water

When the face of a finite solid elastic cylinder is ensonified by an acoustic wave, a variety of backscattering contributions associated with acoustic wave coupling into elastic waves are observed. A significant backscattering enhancement is observed for tilts such that the acoustic wave is incident on the face of the cylinder in the vicinity of the coupling angle for launching Rayleigh waves across the face. The observed backscattering indicates that the Rayleigh waves are reflected at the edge of the face and subsequently radiate acoustic waves in the backscattering direction. The measured backscattering is compared to an approximate theoretical prediction. Approximating the focusing of the Rayleigh wave after reflection at the (circular) edge by a Gaussian beam pressure distribution on the cylinder's face yields simple expressions for the amplitude which are consistent with the measurements. In the vicinity of end-on incidence, other backscattering contributions due to the reflection of waves traveling down the length of the cylinder are observed. There is also evidence of a face-traversing longitudinal wave for slightly tilted cylinders.     

空间频率域超声背散射参量用于骨质状况的评价*

在超声背散射骨质评价中,不同测量感兴趣区域(ROI)的超声背散射信号会有波动,致使诊断准确度降低。该文目的是研究超声背散射信号随测量区域的变化规律。采用空间扫描方法离体测量了35块骨样本,将超声背散射参数从空间域变换到空间频率域。结果表明,超声背散射参数的主要空间频率成分集中于低频部分;空间频率域超声背散射参量最大值(MASF)与骨矿密度等参数具有中高度显著相关性(R2=0.45~0.83,p0.001);空间频率域超声背散射参量衰减系数(AC)也与松质骨密度及结构特征有显著相关性(R2=0.41~0.72,p0.001)。研究表明空间频率域变换方法有助于明确超声背散射信号随测量ROI的变化规律,空间频率域的超声背散射相关新参量评价松质骨状况具有可行性。     

强壮前沟藻的后向散射特性研究

基于2012年7月藻类培养实验期间的实测生物-光学数据,分析了强壮前沟藻的后向散射特性及其影响因素。结果表明,强壮前沟藻的后向散射系数值具有光谱变化性,并随叶绿素浓度的升高而增大,两者之间呈很好的幂函数关系,相关系数R2最小值可达0.96;此外,由于色素的吸收作用,使得其光谱形状会随叶绿素的变化而变化;同时获得的后向散射比率620 nm处的变化范围在0.006 4～0.011 6之间;总体上,各波段颗粒物后向散射比率也呈现随叶绿素浓度增加而增大的趋势,但在高叶绿素浓度下,这种变化规律并不明显,并且就其光谱形状而言,无论叶绿素浓度高低,其光谱形状始终保持一致;颗粒密度是影响后向散射比率的主要因素之一,两者之间呈幂函数关系,相关系数r在620 nm处高达0.98。     

Electromagnetic backscattering from one-dimensional drifting fractal sea surface Ⅱ:Electromagnetic backscattering model

Sea surface current has a significant influence on electromagnetic(EM) backscattering signals and may constitute a dominant synthetic aperture radar(SAR) imaging mechanism. An effective EM backscattering model for a one-dimensional drifting fractal sea surface is presented in this paper. This model is used to simulate EM backscattering signals from the drifting sea surface. Numerical results show that ocean currents have a significant influence on EM backscattering signals from the sea surface. The normalized radar cross section(NRCS) discrepancies between the model for a coupled wavecurrent fractal sea surface and the model for an uncoupled fractal sea surface increase with the increase of incidence angle,as well as with increasing ocean currents. Ocean currents that are parallel to the direction of the wave can weaken the EM backscattering signal intensity, while the EM backscattering signal is intensified by ocean currents propagating oppositely to the wave direction. The model presented in this paper can be used to study the SAR imaging mechanism for a drifting sea surface.     

水下激光探测系统的水体后向散射光计算与光学参数估计

针对水下激光探测系统的水体后向散射光的计算,给出了系统的光学几何结构,分析了不同距离处的激光光斑与接收视场区域的位置变化关系并进行了定量计算。依据光传输理论建立了水体后向散射光的计算模型,根据模型的算法步骤编写了计算机程序。结合水下激光探测系统的具体参数进行了实例计算,绘制了后向散射光信号波形,并与试验获取的信号波形对比分析,验证了算法的可行性和正确性。研究了使用实测后向散射光信号数据估计水体光学特性参数的方法,通过估算的参数重新绘制曲线并反向叠加在测量数据曲线上以抵消水体后向散射光对目标信号的影响从而能够提取目标信息。     

有监督学习的超声背散射方法在骨质评价中的应用

在超声背散射方法评价骨质的实际应用中,如何更为准确地判断测量对象是否为骨质疏松是一个重要问题。提出一种有监督学习的超声背散射评价方法,根据超声背散射离体实验的信号处理结果,对松质骨样本使用支撑向量机和自适应增强的有监督学习算法进行预测和分类。研究结果表明,有监督学习的超声背散射评价方法分类的准确率为80.00%~82.86%,并且对骨质疏松的样本具有较高的特异性(特异度>92.3%)。因此有监督学习的超声背散射评价方法具有有效性,评价效果优于现有的其它定量超声方法,对超声背散射方法的在体应用有一定帮助。      

Coherent backscattering of light in nematic liquid crystals

Multiple light scattering by director fluctuations in nematic liquid crystals is considered. A uniform director orientation is assumed to be specified by an applied magnetic field. The coherent backscattering effect, which consists in the presence of a sharp light backscattering peak, is studied. The Bethe-Salpeter equation is used to calculate the multiple scattering intensity taking into account the contributions of ladder and cyclic diagrams. An analytical expression for the angular and polarization dependences of the coherent backscattering intensity is obtained in terms of the diffusion approximation. The calculation and experimental results are compared. The developed theory is shown to qualitatively describe the elliptical shape of the backscattering cone, to explain the absence of a coherent contribution for crossed polarizations, and to calculate the relative peak height.     

气泡幕后向散射光信号特性的蒙特卡罗方法研究

利用蒙特卡罗方法对水介质中的气泡幕的后向光散射回波信号进行了系统仿真。通过对计算结果与实验结果的比较,证明了蒙特卡罗方法的有效性。根据仿真结果,结合理论分析的方法,对气泡幕位置、厚度和接收器视场角等参数对回波信号的影响进行了分析,结果表明:回波信号出现时间与气泡幕位置存在一一对应的关系;在气泡幕的衰减系数ρσt不变的情况下,存在一个有效气泡幕厚度,当大于该厚度时,气泡幕的后向光散射回波信号基本不变;在系统各项参数不变的情况下,适当增加接收器的视场角,可有效地提高回波信号的信噪比。     

H+2，H+3团簇离子在沟道条件下的背散射 质子产额测量

采用卢瑟福背散射方法，测得了每质子能量为650 keV的H⁺₂，H+₃团簇离子在Si晶体<100>和<110>沟道条件下的质子背散射能谱.结果发现，由于H⁺₂，H⁺₃团簇在晶体中的库仑爆炸和团簇效应，H⁺₂的背散射质子产额大于H ⁺的背散射产额，而H^{+< 关键词： 团簇 沟道效应 库仑爆炸 背散射}     

C-band scattering simulation of a Scots pine shoot

Scots pine (Pinus sylvestris L.) has the widest distribution of any pine and is one of the most important timber trees in Europe and one of the main species of boreal forest, which have an important role in climate change studies. The leaf area index (LAI) is one of the key input parameters for the climate change models. Recently a relationship between C-band backscattering and the LAI has been detected for Scots pine. To understand the C-band microwave characteristics of Scots pine shoots the backscattering is simulated using the so-called discrete dipole approximation (DDA), which is the only possible, nearly exact method for this problem. The backscattering of the shoot is dominated by the needles. The VV/HH backscattering ratio of closely spaced parallel and perpendicular shoots averages to that of a single shoot. For a simulated whole Scots pine crown the VV/HH backscattering ratio is related to the total orientation distribution of the needles. The variation range of the VV/HH backscattering ratio was 0.95-1.25, which is close to empirical values.     

Effect of backscattering on the behavior of a dye ring laser

The effect of backscattering on the behavior of a dye ring laser is investigated by photoelectric counting measurements. It is found that there exist two laser regimes, a low backscattering regime in which the laser exhibits meta-bistability and random mode switching, and a high backscattering regime in which switching is suppressed. In the latter case the photon statistics are similar to those of a single-mode standing wave dye laser.