群聚球形粒子极化散射的T矩阵数值模拟

对于不小于波长或可与波长相比的大粒子集合性的相干散射,要求严格求解多次散射的Maxwel方程。作者利用多个粒子多次散射的严格的T矩阵公式,发展了数值模似算法,求出非均匀群聚分布的球形粒子相干极化散射在全方位上的数值结果,研究了群聚粒子相干极化散射的特征表现,并与双球粒子散射的实验结果作了很好的比较。     

链式生物分子电磁(光)散射的T矩阵方法

具有生物蛋白酶主要功能的较小型分子集团的酶模型的人工设计,是生物有机化学家的重要研究方向。通过非接触、非破坏性的电磁散射的方法对物质结构特性进行研究是物理学的常用方法。本文模拟了具有Koch曲线形式的分形链式结构。用T矩阵的方法,研究了该分子集团的电磁散射特性。对这一不同领域的研究问题进行了有益的尝试。     

基于递归T矩阵的离散随机散射体散射特性研究

本文根据电磁场矢量球波函数多极点展开原理及矢量叠加定理提出了递归T矩阵算法的矢量形式,并且基于矢量递归T矩阵算法建立了多散射球模拟离散随机散射体散射的三维电磁散射模型.通过计算不同尺寸、随机分布散射球的散射以及分析散射球间的高阶散射效应,结果表明:矢量递归T矩阵算法具有很高的计算精度,算法中包含多散射体间的高阶散射效应,因此能够精确计算多散射体总的散射效应.本文所建模型可应用于土壤湿度探测工程中评估地表下掩埋离散随机散射体散射对雷达回波信号产生的影响.     

一种半导体表面上微粒缺陷散射场的计算方法

本文通过分析半导体表面上微粒缺陷散射场的光波传播规律,建立了表面上微粒缺陷场的传输模型和数学模型,使定量计算表面上微粒缺陷的散射场成为可能。进一步将入射场和散射场都表达成球矢量波函数的形式,并考虑表面的二次散射作用,用T矩阵将入射场和散射场的展开项系数连系起来。从而得到散射场与入射场之间的一系列定量表达式,并给出计算结果。     

光散射聚集速率测定中T矩阵方法的应用

聚集速率是评估胶体体系特性及稳定性的关键参数, 静态光散射和动态光散射则是测量聚集速率的两个重要方法. 然而, 用静态光散射和动态光散射测量聚集速率时, 需要知道有关单粒子和双粒子聚集体光散射特性的数据. 为此, 通常需要把动、静两种方法结合, 才能消去这个数据. 以前各种近似理论曾用来解决这个问题, 但因粒子尺寸和形状的限制, 结果并不理想. 而T矩阵方法可以不受粒子大小和形状的限制计算其光散射特性. 本工作用T矩阵方法直接计算静态光散射和动态光散射所必须的粒子散射特性, 并将该法得到的聚集速率与动静态光散射结合法得到的聚集速率进行了比较, 两者结果很接近. 本工作为简化静态光散射和动态光散射测量聚集速率, 扩展其应用范围开辟了新途径. 关键词： T矩阵')" href="#">T矩阵 光散射法 聚集速率     

非球形烟尘粒子后向散射场的光谱分析

在利用后向散射法测量烟尘浓度和粒径的过程中,对烟尘粒子模型的后向散射光谱特性进了计算,确定影响后向散射光谱强度的主要因素并进行分析。对实际排放的烟尘进行显微观察表明,利用椭球、圆柱和广义切比雪夫3种非球模型可以较好地模拟烟尘粒子,其等效直径约1μm。通过"T矩阵法"对这3种非球形粒子模型后向散射场的光谱特性进行了分析,结果表明:非球形粒子的可见/红外波段后向散射现象较球形粒子明显,特别是广义切比雪夫粒子的后向散射光强最高可达到前向的3.5倍;对于吸收性非球形粒子(复折射率m=1.57-0.56i),后向散射光强远大于非吸收性非球形粒子(复折射率m=1.57-0.001i);随着粒子等效半径的增大,光源波长也应随之增加。这为在实际测量时光源及方位的选择提供了理论依据。     

散射场展开项中截断系数N取值的考虑

本文讨论了用T矩阵求解散射场时,散射场展开项截断系数n取值的问题。取值的原则是既要保证T矩阵方法的计算精度也要保证计算的收敛性。     

基于数字微镜器件超像素法实现散射介质传输矩阵的自参考干涉测量

散射介质的传输矩阵系统描述了散射介质对输入与输出光场之间的变换关系,是研究与控制光在无序介质中传输特性的重要工具.本文使用数字微镜器件实现散射介质传输矩阵的自参考干涉测量,首先利用超像素法实现对入射光的复振幅调制获得同时包含参考光和信号光的复合场,进而基于四步相移法分别测量了散射介质在Hadamard基和轨道角动量(OAM)基下的传输矩阵.进一步,根据相位共轭原理实现了光透过散射介质后的单点聚焦、多点聚焦以及涡旋聚焦,验证了传输矩阵测量的准确性.该方法能够有效提高光场调制的自由度,实现散射介质传输矩阵的测量,对散射环境下的光学成像和光通信等具有潜在应用价值.     

结合n模式表示势的含时密度矩阵重正化群求解激发态非辐射衰减速率：理论形式和在薁分子中的应用

本文提出一种来计算多原子分子包含Franck-Condon区势能面非谐效应的无辐射衰减速率的方法. 这种方法结合了n模式表示法,通过构造第一性势能面和近乎精确的含时密度矩阵重正化群法(TD-DMRG),来模拟量子动力学过程. 另外,在TD-DMRG 的框架下,进一步发展了计算末态分辨的速率常数的算法,它对于分析每个振动模式对于跃迁过程的贡献十分有用. 本文采用这种方法研究了考虑基态势能面非谐性后的薁分子的内转换过程. 结果表明,即使对这个半刚性的分子,模式内的非谐性也能够显著的提高内转换速率;在考虑双模式的耦合之后,速率会进一步增加. 其原因是由于C-H振动的黄昆因子接近于0,其在简谐势能面上无法对内转换做出贡献,而非谐性打开了C-H振动接受电子能量的能力.     

Scattering of a Generic Two-Dimensional Field by Cylindrical Structures in the Presence of a Plane Interface

A new method for treating the scattering of a two-dimensional electromagnetic field, expressed by means of its plane-wave spectrum, by an arbitrary configuration of circular cylinders in the presence of a plane interface between two different media, is presented. The proposed method allows us to solve the problem for both polarizations and to calculate the scattered field both in the near and in the far zone. Numerical results relevant to vacuum-dielectric interfaces are presented and compared with previous known results.     

强场中NO分子回归谱的长程散射矩阵的理论研究

采用半经典散射矩阵方法研究外磁场中高里德伯态双原子分子在能量范围为77010—77050cm^-1的回归谱.通过引进模型势简化强磁场中NO分子的高里德伯电子的势函数,找出其在核转动量子数分别为N=1,3,5的三个通道中的闭合轨道,重点分析了强磁场中NO分子的长程散射矩阵元实部的傅里叶变换谱与闭合轨道之间的一一对应关系.     

Amplification Spectra Under the Conditions of Narrow-Band Pumping and in Probing by a Trial Field

The processes of parametric interaction in different techniques of organization of the effect of laser radiation on the resonant transitions of the vapors of alkali metal atoms have been investigated experimentally and theoretically. The results obtained show that, provided there are processes of four-wave mixing under the resonance conditions, it is necessary to consider the structure of the quasi-levels that are formed on exposure to the pumping-field narrow-band radiation. Based on the two-level model, a nonlinear theory of resonant frequency-nondegenerate mixing of arbitrary-intensity waves has been developed that describes the spectral regular and energy characteristics of parametric scattering. __________ Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 72, No. 5, pp. 598–603, September–October, 2005.     

The Solution of a New Kind of Integrals of Bessel Functions Used in the Power Calculation

In the evaluation of the power flow in some millimeter RF structures, a new kind of integrals of the type in which _±(kr) denotes arbitrary Bessel functions of real order ±, is met. In order to integrate it, a new transformation of modified Bessel function is build in this paper: then a general integral formula involving the products two terms, each of them can be expressed a sum of any two modified Bessel function, is obtained by means of applying a theorem on calculus to this transformation smartly, Furthermore, making use of the characteristics of modified Bessel function and the definition of Bessel function, the analytical expression of the above integral is derived.     

IR Fourier Spectroscopy in Vivo of Human Skin during Its Ablation on Exposure to YAG:Er Laser Radiation and Polarization of the Light Scattered by the Integument

We consider the possibility of monitoring the process of human skin ablation on exposure to pulsed IR laser radiation with the use of the polarization and IR Fourier spectroscopy of disturbed total internal reflection. The laws of the change in the content of water and proteins in the surface layers of skin as a result of cyclic laser effect have been discovered. The interrelation between the degree of polarization of the backward scattered probe radiation with the wavelength corresponding to the maxima of absorption of an oxygenated form of hemoglobin and the index of erythema occurring due to laser action has been established.     

费米-费米散射长度对费米超流气体在幺正极限区域的隧穿现象影响

运用双势阱模型通过调节费米-费米散射长度研究了超流费米气体在幺正极限区域的隧穿现象. 研究发现费米-费米散射长度对量子隧穿效应有显著的影响. 在确定的区域, 可以得到在双势阱中完全的量子隧穿现象, 而在另一些区域, 这种隧穿就完全消失. 由于在实验室中超流费米气体的散射长度是可以调节的, 所以在实验上可以实现通过调节散射长度来控制超流费米气体的宏观隧穿现象.     

在有机蛋白质分子系统中由Pang's孤立子引起的Raman散射的特征

本文从理论上研究了在有机蛋白质分子中由结构畸变和局域涨落引起的 Pang's 孤立子产生的 Raman 散射的特性;给出了这种散射的微分散射截面;得到了一些有意义的结果。     

The influence of anisotropic scattering on the radiative intensity in a gray, plane-parallel medium calculated by the DRESOR method

Even though there have been many ways to treat complex anisotropic scattering problems, in most of the cases only the radiation flux or its dimensionless data were provided, and radiative intensity with high directional resolution could merely be seen. In this paper, a comprehensive formulation for the DRESOR method was proposed to deal with the anisotropic scattering, emitting, absorbing, plane-parallel media with different boundary conditions. The method was validated by the data from literature and the integral formulation of RTE. The DRESOR value plays an important role in the DRESOR method, and how it is determined by the anisotropic scattering was demonstrated by some typical results. The intensities with high directional resolution at any point can be given by the present method. It was found that the scattering phase function has little effect on the intensity for thin optical thickness, for example, 0.1. And there is the largest boundary intensity for the medium with the largest forward scattering capability, and the smallest one with the largest backward scattering capability. An attractive phenomenon was observed that the scattering of the medium makes the intensity at boundary can not reach the blackbody emission capability with the same temperature, even if the optical thickness tends to very large. It was also revealed that the scattering of the medium does not mean it cannot alter the magnitude of the energy; actually, stronger scattering causes the energy to have more chance to be absorbed by the medium, and indirectly changes the energy magnitude in the medium. Finally, it is easy to deduce all the associated quantities such as the radiation flux, the incident radiation and the heat source from the intensity, just as done in literature.