Polarization anisotropy of optical transmission in opals and Langmuir-Blodgett crystals

The transmission spectra of thin-film colloidal photonic crystals with three-dimensional and one-dimensional-two-dimensional photonic energy band structures, i.e., opals and Langmuir-Blodgett crystals with a refractive index contrast of ∼1.5: 1.0, have been measured in linearly polarized light. It has been demonstrated that the polarization anisotropy in the light transmitted through the crystal is uniquely related to the diffraction resonance and that the degree of polarization can exceed 90%. A higher degree of polarization is provided by lattices that are characterized by a smaller attenuation of light polarized in the plane of incidence. It has been revealed that the diffraction resonances from the crystal planes for which the dispersions are in anticrossing with the dispersion of the growth planes acquire the same anisotropy. The general character of the results obtained has been confirmed by the fact that the polarization anisotropy identically manifests itself in colloidal crystals that have different symmetries and lattice orderings.     

Control of light polarization by acousto-optic diffraction from leaky acoustic wave in LiNbO₃

The acousto-optic control of light polarization due to diffraction by leaky acoustic waves in ZX-LiNbO? has been demonstrated. The randomly polarized light of 633 nm wavelength is converted by the anisotropic diffraction into two beams with mutually orthogonal polarizations, the relative intensities of which depend on the light incidence angle and acoustic frequency. Variation in acoustic frequency from 108 to 112 MHz rotates the polarization of the output optical beam by 90°. The acousto-optic control is accomplished entirely by electronic means and can be applied for implementation of fast polarization converters.     

一种分焦平面偏振成像系统光源标定方法北大核心CSCD

水下偏振成像技术是目前水下成像研究的热点,由于自然光在水中衰减大,水下成像系统多采用主动照明方式。针对分焦平面偏振成像系统中偏振照明光源与偏振探测像元偏振方向不匹配引起采集图像偏振信息存在的偏差,进而影响目标图像增强质量的问题,提出了一种分焦平面偏振成像系统光源标定方法。阐述了偏振光源的标定原理,然后给出偏振光源标定的实施步骤,最后采用偏振去雾算法和图像质量评价方法对标定前后的水下目标图像进行了图像增强和图像质量评价。评价结果表明,标定后的增强图像质量优于未标定的增强图像质量,平均梯度最大提升了2.48倍。该标定方法简单有效,实用性强,适用于分焦平面偏振成像系统偏振光源标定。     

基于AirMSPI多光谱多角度传感器的地物偏振特性研究

偏振是电磁波的重要特性,利用偏振信息研究地物的状态和性质被证明是一种有效的手段。地物属性研究是地球观测中重要的课题,偏振技术作为一种新兴手段,逐渐得到国内外遥感界的关注。目前,国际上普遍缺乏使用广、精度高的偏振传感器。AirMSPI(Airborne Multiangle Spectro Polarimetric Imager)作为新型机载偏振传感器,能够获取多波段多角度的偏振数据,空间分辨率可达10 m。选取2013年美国Tracy地区的航飞数据,分析了线偏振度(degree of linear polarization,DOLP)与偏振二向反射因子(polarized bidirectional reflectance factor,pBRF)在470,660和865 nm三个波段、九个探测天顶角的变化规律。研究发现,地物前向散射方向包含大量偏振光,其在入射主平面附近表现出强烈的非朗伯体效应。同时,DOLP与pBRF和入射天顶角及探测天顶角的相对位置有关。DOLP在入射及探测天顶角90°夹角附近最大,pBRF随着探测天顶角的增大而增大。受大气影响,蓝光波段的DOLP及pBRF数值相对较高,但红光及近红外波段可有效减弱大气分子偏振散射效应,包含更多地物偏振细节。水体、人工建筑、居民区、裸土和绿地偏振特性迥异,偏振图像中地物甄别度高。且由于分子多次散射的退偏作用,传感器接收到的地物辐射中,线偏振度与反射比具有高度负相关性,相关系数普遍大于-0.8。因此,AirMSPI能够提供高质量偏振数据,作为地面、星载偏振数据的有力验证,为大气及地物参数反演提供重要支持。     

Scattering of on-axis polarized Gaussian light beam by spheroidal water coating aerosol particle

Small particle light scattering can produce light with polarization characteristics different from those of the incident beam. An analytical solution to the scattering by a spheroid with inclusion for an on-axis polarized Gaussian beam incidence is provided within the generalized Lorenz-Mie theory framework. The shapes of the inclusion can be spherical, confocal spheroid, or non-confocal spheroid. The Muller scattering matrix elements are computed for plane wave incidence or Gaussian light beam incidence. The effect of the size and shape of the inclusion or the coating on the polarized Oaussian light scattering characteristics by a spheroidal water coating aerosol Darticle are commlted and a,nalvzed.     

On vector radiative transfer equation in curvilinear coordinate systems

The differential operator of polarized radiative transfer equation is examined in case of homogeneous medium in Euclidean three-dimensional space with arbitrary curvilinear coordinate system defined in it. This study shows that an apparent rotation of polarization plane along the light ray with respect to the chosen reference plane for Stokes parameters generally takes place, due to purely geometric reasons. Analytic expressions for the differential operator of transfer equation dependent on the components of metric tensor and their derivatives are found, and the derivation of differential operator of polarized radiative transfer equation has been made a standard procedure. Considerable simplifications take place if the coordinate system is orthogonal.     

任意偏振态光束全反射时的侧向和横向位移

光束在电介质界面发生全反射时,实际反射光束会在入射面内相对于几何反射光束产生一侧向位移,在垂直于入射面的方向产生一横向位移。利用改进的能流法研究了任意偏振态光束发生全反射时的侧向和横向位移特性。研究表明,侧向位移的大小与入射光束的两组成部分———TE和TM偏振光的相位差无关,而与两组分的光强比密切相关,且该位移可以表示为TE和TM偏振光束各自的位移按光强的加权平均。横向位移的大小不仅与入射光束两组分的光强比相关,还与组分的相位差密切相关。另外,反射光束不仅在椭圆偏振态入射的情况下会产生横向位移,而且在TE和TM偏振态之外的其他线偏振态入射时,也会产生横向位移。     

Recent Studies of the Circular Dichroism and Optical Rotatory Dispersion of Biopolymers

When electromagnetic radiation interacts with matter, a number of changes result both in the light and in matter. The intensity of the light at given wavelength may be reduced due to absorption; the velocity of light may change, dependent on the wavelength, upon interaction with the medium due to refractive index dispersion (scattering). If the incident light is plane polarized, a change in the plane of polarization may occur, again dependent on wavelength [optical rotatory dispersion (ORD)]. Also, the radiation may become elliptically polarized at the absorption bands; this phenomenon is termed circular dichroism (CD). While normal absorption and dispersion occur with any molecule, ORD and CD require not only polarized light but also molecular systems with built-in asymmetry or dissymmetry.     

纳米ZnO薄膜的反射及偏振特性研究

用电子束蒸发镀膜法制备了纳米ZnO薄膜．通过测量其X射线衍射谱,计算出纳米ZnO颗粒的平均粒径大小为30nm．实验研究了纳米ZnO薄膜的反射和偏振性质,结果表明：当振动方向平行于入射面的线偏振光（简称P光）入射纳米ZnO薄膜时,不存在严格意义上的布儒斯特角,但对于入射角却存在一个临界角β．当入射角小于β时,反射光的振动面随着入射角的增大向左旋转;当入射角大于β时,振动面转而向右旋转;当振动方向垂直于入射面的线偏振光（简称S光）入射纳米ZnO薄膜时,反射光的振动面始终向左旋转．     

Single layer homogeneous model for surface roughness by polarized light scattering

In this paper a homogeneous single layer model for surface roughness by polarized light has been developed. It has been shown that the reflectance change in non-absorbing layer is directly proportional to the refractive index of the ambient and substrate media for s polarization but inversely proportional to the p polarization and it is directly proportional to the square of the thickness of the layer for both the polarization. In an absorbing layer, it has been shown that the thickness of the layer is equal to the twice of surface roughness of the single layer identical system for s polarization but it is ratio of twice of surface roughness to the square of refractive index of thin film for p polarization. The extinction coefficient of the layer is directly proportional to the thickness of that layer for both the polarization. The consequence of the scattered light on the specular reflectance and transmittance for oblique incidence shows that there is reduction in reflectance (in both non-absorbing and absorbing cases) and transmittance (in the absorbing case for p polarization only), due to roughness on the surface under the Drude effective-medium approximation. Thus such an absorbing layer provides a valid model for the effect of scatter on the transmittance for p polarization only.     

利用表面散射光偏振差异的目标识别技术

 分析了不同物体散射场偏振特性的差异,依据消光定理的矢量微扰解方法将物体散射场分为零阶和高阶解,零阶反射光可完全保持入射光的偏振度,高阶散射则会导致偏振度的降低,因而总散射光的偏振度依赖于散射表面的粗糙程度。提出了利用斯托克斯-穆勒体系测量物体消偏特性的方法并通过实验对一些物体作了测量,实验结果表明：光滑表面可以较好地保留入射光偏振度,而粗糙表面则有很强的消偏作用,因此偏振成像方法可有效地提高目标探测和识别效率。     

双色激光偏振演示实验

利用红色和绿色激光束产生2束偏振方向分别平行及垂直于入射面的偏振光,再混合为1束光.通过缓慢改变光束的偏振结构及其与入射透明介质的夹角,使反射与透射光斑颜色及明暗发生变化,演示了马吕斯定律、菲涅耳关系和布儒斯特定律等光的偏振性质.     

Phenomenological interpretation of electroreflectance in gold

Electroreflectance spectra at the gold-electrolyte interface have been investigated at oblique incidence, the light wave being polarized either parallel or perpendicular to the plane of incidence. A new interpretation of the electroreflectance is given, in which this effect is assumed to be due to a surface current related to a change in the electron surface density. The agreement between the theoretical and experimental results is quite good.     

Anisotropic laser-induced evaporation of graphite films

An experimental investigation of the effect of linearly polarized high-energy pulsed laser light, normally incident on a carbon thin film, is reported. The material under study consists of platelike graphite crystallites with basal crystallographic planes mostly oriented perpendicular to the substrate surface. An increase is revealed in the fraction of the graphite crystallites oriented perpendicular to the polarization plane. Laser light is found to cause significant anisotropy in diffuse scattering by the film surface. Experimental observations are explained by a model of anisotropic evaporation of graphite-like carbon material due to polarization dependence of the absorption and reflection coefficients for a rough surface.     

平面偏振光激励的多孔硅的光致发光

研究了以掠入射的平面偏振光激励的多孔硅的光致发光。实验结果显示，光的入射角对多孔硅的发光行为影响不大，然而，以ｚ方向偏振光激励的发光强度明显高于以ｘ方向偏振光激励的发光强度。激励光电场相对于样品表面的不同取向引起光致发光的差异，这反映多孔硅的光学性质是各向异性的，也排除了纯粹的硅量子点的集合作为多孔结构的可能性。     

Bessel beams: Effects of polarization

An approximation to a Bessel beam produced by tightly focusing linearly polarized light is known to produce a smaller central lobe than focusing plane polarized light. This is because the plane polarized wave gives a broad central lobe caused mainly by a parasitic longitudinal field component. It is known that this problem can be overcome by focusing radially polarized light. Here we demonstrate that other polarization distributions based on a linear combination of transverse electric (TE1) and transverse magnetic (TM1) fields can give a beam even narrower than for the radially polarized case. Special cases of this combination are identified, corresponding to the smallest width (TE1), and the maximum peak intensity compared with the side lobes (electric dipole polarization). Axially-symmetric forms can be generated by illumination with elliptically polarized light. A particular case is azimuthal polarization with a phase singularity, which is equivalent to TE1. For a semi-angular aperture of 60°, the TE1 case gives a central lobe width 9% narrower than for radially polarized illumination, while for plane polarized illumination it is 12% wider than the radially polarized case.     

Anisotropy of light propagation in thin opal films

Thin opal films are prepared by crystallization in a moving meniscus, and their optical transmission spectra are recorded in polarized light and studied. It is shown that the anisotropy of light propagation in the films is unambiguously related to the photonic band structure of opal and depends on the angle of incidence, the orientation of the incidence plane with respect to the opal lattice, and the wavelength and polarization of the incident light. Azimuthal diagrams of transmitted polarized light are constructed in the range of photonic band gaps of three orders for oblique incidence of a light beam. The anisotropy is found to vary with the light wave-length independently in perpendicular polarizations. A model of the band structure of opal wherein opal is represented as an fcc lattice of close-packed spheres adequately describes the optical transmission of opal films only in the range of the first-order photonic band gap.     

Subwavelength gratings fabricated on semiconductor substrates via E-beam lithography and lift-off method

We present results of the fabrication and measurements on reflective polarizers consisting of stacked bi-layer subwavelength metal gratings prepared on GaAs (100) substrates. These linear gratings were fabricated using electron-beam direct-writing lithography and the lift-off method with periods less than the wavelength of light used for measurements. At normal incidence, the polarizer reflects the light polarized perpendicular to the grating lines (transverse magnetic polarization, TM polarized) but absorbs parallel-polarized light (transverse electric polarization, TE polarized). By optimizing structural parameters, the polarization extinction ratio close to 20 has been experimentally achieved at wavelength of 650 nm.     

Polarization Dynamics of a Distributed-Feedback Dye Laser

The polarization dynamics of a dye-solution laser with light-induced distributed feedback (DFB) has been analyzed. A theoretical model of a DFB-laser, which makes it possible to calculate the dynamics of the lasing process for two orthogonally polarized modes, has been constructed. The influence of three main factors — rotational diffusion of dye molecules in solution, anisotropy of the saturation effect, and orientation of the electric vector of pumping beams with respect to the plane of their incidence — on the degree of polarization of output radiation has been investigated. Comparison of the calculated dependences with the results of experimental measurements has shown that the latter factor is of the greatest importance. It is shown that in this case, the degree of polarization of the output radiation of a DFB-laser can have a complex dynamics that does not correlate with the time behavior of the lasing pulse.     

Polarization and amplitude optical multistability in a nonlinear ring cavity

The stimulation of a ring cavity filled with an isotropic medium with third order nonlinearity by plane monochromatic arbitrary polarized light is studied. An evolution of the stationary transmission with the change of the polarization of the incident light from circular to linear is discussed. For the linear polarized incident light additional branches of high transmission corresponding to elliptically polarized transmitted light and degenerating with respect to the rotation of the polarization vector are found. The stability of the stationary solutions is discussed. The possibility of the transmitted light polarization and intensity control by changing the polarization ellipticity degree of the incident light is shown.