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1.
用偶极子-自洽场理论模拟计算了反射式近场光学扫描显微镜中入射光的偏振特性对近场成像结果的影响(包括系统分辨率和相关的成像特性),并给予了相应的分析和解释。分析计算结果表明,入射光偏振性的选择将影响近场光学显微镜的成像质量。在近场区域,用垂直于样品表面偏振的入射光(即x方向偏振)照明成像将得到优于相应水平偏振(即x方向偏振)的入射光照明的系统分辨率。用x方向偏振的入射光照明时,所得光学图像会发生局部的光强对比度反转。  相似文献   

2.
吴才章  叶梅  叶虎年 《光子学报》2005,34(10):1546-1549
为了研究扫描近场光学显微镜中探针和粗糙样品表面的耦合相互作用,提出了一种光耦合偶极子模型.在该模型中,探针和样品突起都由光极化偶极子表示,在准静态电磁场近似的情况下样品表面的诱导极化效应由影像偶极子表示,应用偶极子辐射理论可以得到系统的自洽场方程.此模型提供了一种直观分析扫描近场光学显微镜中探针和样品相互作用机理的方法.在此基础上,进一步讨论了金属样品的近场成像特点和其特有的局域光学共振现象.数值结果表明:不同于一般的介质样品,金属样品的近场图像与入射光频率直接相关,改变入射光的频率,获得的样品近场图像的形状和对比度都会发生变化.特别是当入射光频率处于样品极化共振范围内时,金属纳米粒子的极化率会出现光极化共振,这样就可以获得样品粒子的最大有效尺寸,为提高系统的分辨率提供了一条重要途径.  相似文献   

3.
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.  相似文献   

4.
We have gained a very comprehensive set of results for infrared diffraction (10.6 μm wavelength) from fabricated single grooves of reflection with widths in the range of 5μm to 65μm. The experimental results show that the diffraction can still occur when the groove width becomes comparable to or less than the wavelength of the probing light. Variations of the diffraction intensities have a very regular sinusoidal relationship with the polarization angle of the incident light; and the diffraction intensities are the maximal when the incident light is TM polarized. However, the diffraction intensities will be a minimum when the incident light is TE polarized; and the bigger the diffraction angle, the higher the rate of change of the diffractive intensity with increasing polarization angle of the incident light.  相似文献   

5.
与人射线偏振光振动方向无关的低偏振度消偏器   总被引:2,自引:0,他引:2  
消偏器是光纤传感器、光放大器等偏振敏感性光学系统中的关键器件,用于减小输入光的偏振度(DOP)。设计了一种与入射线偏振光振动方向无关的低偏振度消偏器,该器件中利用人为的偏振相关延迟代替了保偏光纤的双折射,并在偏振相关型消偏器前增加了一个1/4波片,从而对任意方向振动的线偏振光具有相同的消偏能力,结构紧凑。对消偏性能随波片阶数、入射光中心波长和振动方向的变化作了数值计算。实验中采用半峰全宽为0.13 nm的光源,入射线偏振光在任意方向振动时,输出光偏振度小于2.6%,消偏器的插入损耗为0.6 dB,损耗起伏小于0.11 dB。实验和数值计算结果表明,该消偏器具有低偏振度、低插入损耗和适合于宽光谱应用的优点。  相似文献   

6.
与入射线偏振光振动方向无关的低偏振度消偏器   总被引:1,自引:0,他引:1  
刘继红  方强  阴亚芳  梁猛  陆蓉 《光学学报》2007,27(3):536-539
消偏器是光纤传感器、光放大器等偏振敏感性光学系统中的关键器件,用于减小输入光的偏振度(DOP).设计了一种与入射线偏振光振动方向无关的低偏振度消偏器,该器件中利用人为的偏振相关延迟代替了保偏光纤的双折射,并在偏振相关型消偏器前增加了一个1/4波片,从而对任意方向振动的线偏振光具有相同的消偏能力,结构紧凑.对消偏性能随波片阶数、入射光中心波长和振动方向的变化作了数值计算.实验中采用半峰全宽为0.13 nm的光源,入射线偏振光在任意方向振动时,输出光偏振度小于2.6%,消偏器的插入损耗为0.6 dB,损耗起伏小于0.11 dB.实验和数值计算结果表明,该消偏器具有低偏振度、低插入损耗和适合于宽光谱应用的优点.  相似文献   

7.
以斯托克斯矢量理论为基础,通过搭建偏振传输半实物模拟装置进行模拟实验,观测激光在模拟环境(不同浓度的椭球粒子在非均匀分布状态)下偏振度(degree of polarization, DOP)的变化。实验选取灵芝孢子碳化粉末作为椭球粒子的实验对象,通过烟雾机将椭球粒子形成不同浓度的烟雾,研究入射波长为532 nm、671 nm的激光在0°、+45°、90°的线偏振光以及左旋圆偏振光经过模拟环境后偏振度(DOP)的变化情况。实验结果表明:入射偏振光随着烟雾浓度的增大,偏振度呈下降趋势;3种入射线偏振光随浓度增大降幅不尽相同,没有明显的规律可循;不同波长低浓度烟雾时,线偏振光与圆偏振光的偏振度下降幅度大抵相同,大约为3%左右;随着烟雾浓度的增大,线偏振光的偏振度表现出不同程度的下降,可达20%,圆偏振光的偏振度仅下降5%,表现出了较好的保偏能力。  相似文献   

8.
Zhao QZ  Malzer S  Wang LJ 《Optics letters》2007,32(13):1932-1934
The evolution of surface morphology of tungsten irradiated by single-beam femtosecond laser pulses is investigated. Ripplelike periodic structures have been observed. The period of these ripples does not show a simple relation to the wavelength and angle of incidence. The orientation of ripples is aligned perpendicularly to the direction of polarization for linearly polarized light. Surprisingly, we find that the alignment of the ripple structure turned left or right by 45 degrees with respect to the incident plane when using right and left circularly polarized light, respectively. The period of the ripple can be controlled by the pulse energy, the number of pulses, and the incident angle. We find a clear threshold for the formation as a function of pulse energy and number of pulses. The mechanism for the ripple formation is discussed, as well as potential applications in large-area structuring of metals.  相似文献   

9.
Lv Y  Wang Z  Jin Y  Cao M  Han L  Zhang P  Li H  Gao H  Li F 《Optics letters》2012,37(5):984-986
A spin polarization separation of reflected light is observed, when a linearly polarized Gaussian beam impinges on an air-glass interface at Brewster angle. In the far-field zone, spins of photons are oppositely polarized in two regions along the direction perpendicular to incident plane. Spatial scale of this polarization is related to optical properties of dielectric and can be controlled by experimental configuration. We believe that this study benefits the manipulation of spins of photons and the development of methods for investigating optical properties of materials.  相似文献   

10.
曹先平  孙萍 《光子学报》2012,41(5):608-613
基于Stockes矢量,通过测量以线偏振光和圆偏振光入射时脂肪乳剂后向散射光的偏振度,研究了532nm、650nm和780nm三个波长的光与散射粒子粒径为325nm的脂肪乳剂溶液作用后,其后向散射光的偏振度特性.研究结果表明,对于入射线偏振光,780nm波长后向散射光中的线偏振光成分多于圆偏振光成分,而532nm波长则相反;对于入射圆偏振光,三个波长后向散射光中的圆偏振光成分均多于线偏振光成分;532nm波长的总偏振度高于650nm和780nm两个波长各自的总偏振度;线偏振光的保偏性优于圆偏振光的保偏性,但偏振光在散射介质中的穿透深度较小.因此,后向散射成像技术适用于物体表层成像,而且选择波长略大于粒径的线偏振光可以提高成像质量.  相似文献   

11.
曹先平  孙萍 《光子学报》2014,(5):608-613
基于Stockes矢量,通过测量以线偏振光和圆偏振光入射时脂肪乳剂后向散射光的偏振度,研究了532 nm、650 nm和780 nm三个波长的光与散射粒子粒径为325 nm的脂肪乳剂溶液作用后,其后向散射光的偏振度特性.研究结果表明,对于入射线偏振光,780 nm波长后向散射光中的线偏振光成分多于圆偏振光成分,而532 nm波长则相反;对于入射圆偏振光,三个波长后向散射光中的圆偏振光成分均多于线偏振光成分;532 nm波长的总偏振度高于650 nm和780 nm两个波长各自的总偏振度;线偏振光的保偏性优于圆偏振光的保偏性,但偏振光在散射介质中的穿透深度较小.因此,后向散射成像技术适用于物体表层成像,而且选择波长略大于粒径的线偏振光可以提高成像质量.  相似文献   

12.
The interaction of linearly polarized light with photonic crystals based on bulk and thin-film synthetic opals is studied. Experimental transmission spectra and spectra showing the polarization state of light transmitted through opals are discussed. A change in polarization is found for waves experiencing Bragg diffraction from systems of crystallographic planes of the opal lattice. It is shown that the polarization plane of the incident linearly polarized wave at the exit from photonic crystals can be considerably rotated. In addition, incident linearly polarized light can be transformed to elliptically polarized light with the turned major axis of the polarization ellipse. Analysis of polarization states of transmitted light by using the transfer-matrix theory and homogenization theory revealed good agreement between calculated and experimental spectra.  相似文献   

13.
用偏振荧光光谱表征乙醇-水团簇分子的取向行为   总被引:1,自引:0,他引:1       下载免费PDF全文
采用波长为236nm紫外光激励乙醇水溶液获得荧光光谱并对其偏振特性进行了研究.实验中分别改变入射光的偏振度,在300—400nm波段内进行荧光光谱、水平和垂直偏振荧光光谱检测.实验结果表明,当采用线偏振光照射乙醇水溶液时,其发射的荧光具有一定的偏振性,并计算了其偏振度.经理论分析得到了描述荧光偏振态的四个斯托克斯矢量,进而对该荧光的偏振状态进行了描述,通过对乙醇-水溶液的米勒矩阵的计算,对溶液中分子的取向特性进行了分析.本结果能对乙醇-水团簇分子的结构提供理论参考. 关键词: 荧光光谱 偏振光谱 斯托克斯矢量 米勒矩阵  相似文献   

14.
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.  相似文献   

15.
D. Venus  M.J.G. Lee 《Surface science》1983,125(2):452-472
The mechanisms of one-photon photoexcitation in photofield emission have been studied experimentally by measuring the photocurrent from selected crystallographic planes of a tungsten field emitter as a function of the polarization of the incident light. Two distinct components of the photocurrent were identified. The corresponding excitation mechanisms were deduced from the results of the polarization measurements supplemented by band structure considerations. Surface effect emission dominates at large angles of light incidence, and is observed even from within the geometric shadow of the tip. It depends on the light polarization inside the metal in a characteristic way. Indirect bulk photoemission is prominent at small angles of light incidence and is independent of the polarization inside the metal. It is concluded that bulk and surface excitations in photofield emission can be distinguished by appropriately selecting the direction of polarization and the angle of incidence of the incident light.  相似文献   

16.
Homeotropically aligned nematic liquid crystals doped with azo-dye were subjected both to a linear polarized light of a He–Ne laser and to a magnetic field perpendicular to the incident light beam. We found that the emerging light was elliptically polarized when using magnetic field strengths higher than the threshold value for the magnetic Freedericksz transition. The light transmission, the rotatory power (induced by azo-dye) and the ellipticity varied quasiperiodically when increasing magnetic field strength. The number and positions of maxima and minima depend on the cell thicknesses. Changes in the phase difference between the emergent ordinary and extraordinary rays were computed from the experimental data and the magnetic field dependence of the birefringence was determined.  相似文献   

17.
Goos-H?nchen(GH)位移是一种特殊的光学现象,具有广泛的应用.构造材料光学性质的差异对同一结构的GH位移有很大影响.在近零介电常数区,本文比较研究了不同偏振态的光波入射到超导薄层上的GH位移.当以大于临界角的入射角入射时,s偏振光的GH位移始终保持为正值,而p偏振光的GH位移的正负与超导材料的介电常数为零时的波长相关联.当入射光波长大于该波长时,GH位移会出现负值.相关参数对不同偏振态下的GH位移的影响存在较大差异.相对于p偏振光,GH位移在s偏振光入射时随相关参数的变化规律较为简单.超导材料在光子学领域具有广泛的应用,计算结果为基于超导材料的新型光子学器件研究开发提供了参考.  相似文献   

18.
The depolarization behavior of backscattered linearly polarized light from ZnO thin film was investigated experimentally. The results show that the characteristics are related to both the polarization orientation and wavelength of linearly polarized incident light. When the incident light is s-polarized, the depolarization behaviors are different for different wavelengths. When the incident light is p-polarized, the depolarization behaviors, on the contrary, are similar for different wavelengths. In addition, there is an optimal incident angle for depolarization of linearly polarized light with different wavelengths, which is equal to their effective Brewster angles, respectively.  相似文献   

19.
The influence of a focused polarized Gaussian beam on image formation was studied. We show that the position of the tip with reference to the center of the beam involves asymmetry in the intensity map. A comparison between s and p polarization can be made, owing to the definition of both a three-dimensional polarized Gaussian beam and a three-dimensional object. This result implies that the best way to scan a sample consists in moving it and not the tip; moreover, focusing the incident light to get a higher signal-to-noise ratio must be done carefully with respect to the sample period.  相似文献   

20.
Quantitative phase microscopy with polarized light has been used to determine the change in refractive index introduced into an optical fiber when the fiber is bent through a constant radius of curvature. By obtaining phase images for two orthogonal directions of the polarization of the incident light, one can infer the induced axial strain profile within the fiber. Radii of curvature from 1 to 8 cm were considered, and in each case excellent agreement, within lambda/100, was obtained between experimental results and theory.  相似文献   

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