Fe:LiNbO_3晶体光折变性能分析计算

掺铁铌酸锂晶体的光折变性能 ,一方面取决于晶体材料制备时的工艺条件和参数 ,另一方面和记录光路布置及晶体光轴的选取密切相关。给出了常用的 90°记录光路中光折变晶体折射率调制度的计算方法和公式 ,并分析了写入光的偏振方向、晶体光轴 (C轴 )方向及全息图折射率调制度之间的关系。     

Astigmatism of the radiation of semiconductor stripe-geometry lasers

The effect of injection current on the intensity and angular distribution of radiation in TE- and TM-polarized modes of diode lasers with a stripe geometry and double GaAs-AlGaAs-based heterostructure is investigated. The analysis of the angular distribution of radiation revealed the nonmonotonic behavior of its astigmatism with increase in the current. The coefficient of astigmatism in the mode of lasing is substantially higher for the TE-mode than for the TM-mode. An increase in radiation astigmatism is accompanied by a decrease in the differential effectiveness and polarization degree. These specific features are explained by the interaction of the defocusing action of distribution of the refractive index n(x) in the plane of the p-n-transition with a minimum under the center of the stripe contract (at x=0) with the focusing action of the gain coefficient distribution. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 67, No. 4, pp. 461–464, July–August, 2000.     

亮孤子在宇称时间对称波导中的传输和控制

基于光波在宇称-时间(PT)对称波导中传输的理论模型, 数值研究了亮孤子在呈高斯分布的PT对称克尔非线性平板波导中的传输和控制. PT对称波导, 要求波导的折射率分布呈偶对称, 而增益/损耗分布呈奇对称. 结果表明: 当波导的折射率分布强度为正时, PT对称波导的中心折射率最大, 即使没有自聚焦克尔非线性效应, PT对称波导也可以束缚光波, 形成波浪形光束且长距离传输; 当折射率分布强度为负时, PT对称波导的中心折射率最小, 光波的传输方向发生偏移. 而增益/损耗分布可控制光波的偏移方向: 增益/损耗分布强度为正, 光波向左偏移; 强度为负, 光波向右偏移; 强度为零时, 光波被分为两束. 且当折射率分布强度为负时, 可以很好地抑制相邻亮孤子间的相互作用. 该研究结果可为未来PT对称波导在全光控制方面的应用提供一定的理论依据.     

手性负折射率材料的最新进展

阐述了手性负折射率现象的产生机制;总结了近几年国内外手性负折射率材料在仿真模拟和实验制备方面的研究进展;分析了手性负折射率材料的旋光性、手性参数、损耗等;介绍了手性负折射率材料在各个领域的应用。分析认为,探索手性负折射率材料的新机制、新方法和新材料,从而在可见光波段实现负折射率是未来手性负折射率材料的重要发展方向之一。     

折射率正负梯度交替表面的研究

利用不均匀材料提出了一种折射率正负梯度交替表面, 并利用几何光学法和电磁场数值仿真方法对其机理进行了研究与验证, 发现其可以操控电磁波的传播: 在一定的参数下, 其可以将空间中的入射电磁波一直束缚在介质中, 或在介质中传播一定距离后再实现电磁波的释放; 同时该结构具有宽带、极化无关等特性. 利用该结构可引导能流, 减小后向散射截面, 可用作隐身表面.     

聚合物分散液晶光栅的衍射特性的研究

报道了一种由聚合物分散液晶膜与具有周期性条状电极结构板结合的新型光栅器件，借助于聚合物分散液晶膜的电光特性，这种栅对入射光的散射或衍射取决于对其施加的电压，即它是电场可调的，实验结果显示出当驱动电压超过器件器件阈值电压时，衍射光的强度和衍射斑的可见级次被电场调制，而且它能入射光的线性偏振态变为椭圆偏振态。     

一种精确测量液体折射率的方法

本文介绍了一种在迈克尔逊干涉仪光路加入一楔形样品池进行液体折射率测量的方法。     

Hydrogen adsorption on Mo1−xRex(110) (x=0–0.25) surfaces

The effects of adsorbed H on the Mo_1−xRe_x(110), x=0, 0.05, 0.15, and 0.25, surfaces have been investigated using low-energy electron diffraction (LEED) and high-resolution electron energy loss spectroscopy (HREELS). For the x=0.15 alloy only, a c(2×2) LEED pattern is observed at a coverage Θ0.25 ML. A (2×2) pattern is observed for H coverages around Θ0.5 ML from surfaces with x=0, 0.05, and 0.15. Both c(2×2) and (2×2) patterns are attributed to reconstruction of the substrate. At higher coverages, a (1×1) pattern is observed. For the alloy surface with x=0.25, only a (1×1) pattern is obtained for all H coverages. Two H vibrations are observed in HREELS spectra for all Re concentrations, which shift to higher energies at intermediate coverages. Both peaks exhibit an isotopic shift, confirming their assignment to hydrogen. For Re concentrations of x=0.15 and higher, a third HREELS peak appears at 50 meV as H (D) coverage approaches saturation. This peak does not shift in energy with isotopic substitution, yet cannot be explained by contamination. The intrinsic width of the loss peaks depends on the Re concentration in the surface region and becomes broader with increasing x. This broadening can be attributed to surface inhomogeneity, but may also reflect increased delocalization of the adsorbed hydrogen atom.     

Photoelectron diffraction study of a catalytically active overlayer: C2H2 on Pd{111}

A quantitative structure determination of a newly discovered (2×2) adsorption phase of acetylene chemisorbed on Pd{111} has been performed by scanned-energy mode photoelectron diffraction: this phase corresponds to the threshold coverage for the catalytic conversion of acetylene to benzene. The carbon atoms in the C₂H₂ molecule are located almost over bridge sites with a C–C bond length of 1.34+0.10 Å, the centre of the molecule being positioned almost over a hollow site. Of the two hollow sites the hcp site (directly above a second layer Pd atom) is favoured, particularly by a subset of the data most sensitive to this aspect of the structure, but the full analysis indicates that the fcc site (above a third layer Pd atom) cannot formally be excluded. The adsorption site adopted by acetylene in the higher coverage phase on Pd{111} is essentially identical. This is the dominant structure in the coverage regime which is catalytically active for the conversion of acetylene to benzene. The implications of these findings for acetylene coupling reactions over Pd{111} are discussed.     

2.0~5.5 GPa压力下合成的SiO2玻璃

 在温度为355～445 ℃、压力为2.0～5.5 GPa条件下，用光谱纯SiO₂合成了一系列SiO₂玻璃，它们的红外光谱谱带特征与高密度石英玻璃相似。SiO₂玻璃和高密度石英玻璃的折光率与压力的对数之间呈线性关系。SiO₂玻璃中含有少量的水，并且以OH^-离子的形式存在。可能正是由于少量的水对SiO₂的非晶化起了重要作用。