类氦离子V21+精细能级结构及跃迁光谱的相对论计算

采用加轨道极化修正的相对论多组态Dirac-Fock方法,计算了类氦离子 V21+的跃迁几率和跃迁波长,所得结果与实验值吻合,比较了极化对能级、能级间隔 和不同类型跃迁的影响,并讨论了轨道极化修正函数。     

晶体CsMnBr_3的自旋极化MS-X_α计算

本文采用自旋极化MS一X_α方法,在晶体CsMnBr_3实际的D_(3d)低对称晶场下计算了络离子(MnBr_6)~(4-)的电子结构.给出了单电子的本征值、本征函数和自旋极化分裂,用过渡态理论计算了部分光学跃迁和电荷转移跃迁的能量,并用Case-Karplus电荷分配法计算得到自旋-轨道耦合常数ξ和讨论了晶体吸收光谱的精细结构.     

类氦离子Cr~(22 ) 精细结构能级和光谱跃迁的相对论多组态计算

采用相对论多组态自洽场方法,计算了类氦Cr22 离子的精细结构能级,能级宽度,激发态寿命和光谱跃迁参数。计算中考虑了核的有限体积效应,Breit修正,QED修正和轨道极化效应。所得结果与文献的实验值和计算值进行了比较     

类锂体系(Z=11～20) 1s~24s -1s~2np(5≤n≤9)跃迁能和振子强度的理论计算

利用全实加关联的方法计算类锂体系(Z=11～20) 1s~24s -1s~2np(5≤n≤9)的跃迁能, 将相对论效应(电子动能的相对论修正,Darwin项,电子-电子接触项以及轨道-轨道相互作用)和质量极化效应作为微扰,计算了它们对体系能量的修正.利用得到的波函数和跃迁能计算了核电荷Z=11~20的类锂离子的1s~24s -1s~2np(5≤n≤9)偶极跃迁的长度、速度和加速度三种规范下的振子强度,与现有的实验数据比较,结果符合得很好.     

类锂体系(Z=1120) 1s24s -1s2np(5≤n≤9)跃迁能和振子强度的理论计算

利用全实加关联的方法计算类锂体系(Z=11~20) 1s24s -1s2np(5≤n≤9)的跃迁能, 将相对论效应(电子动能的相对论修正,Darwin项,电子-电子接触项以及轨道-轨道相互作用)和质量极化效应作为微扰,计算了它们对体系能量的修正．利用得到的波函数和跃迁能计算了核电荷Z=11~20的类锂离子的1s24s -1s2np(5≤n≤9)偶极跃迁的长度、速度和加速度三种规范下的振子强度,与现有的实验数据比较,结果符合得很好.     

半导体量子点中极化子的跃迁能量

研究了半导体量子点中极化子的激发态性质。采用Huybrechts线性组合算符和幺正变换方法,计算了量子点中极化子的振动频率、基态能量、第一激发态能量、由第一激发态向基态的跃迁能量和跃迁频率。分别讨论了电子-LO声子在强弱两种耦合情况下极化子的跃迁能量和跃迁频率。数值计算结果表明,跃迁能量ΔE和跃迁频率ω均随量子点有效受限长度l₀的增加而减少,且随电子-声子耦合强度α的增加而减少。     

用推广的平面波展开法检验平面内极化的电子子带跃迁

把平面波展开包络函数的方法推广到求解8带的哈密顿量，使它同时包括Γ^c₁和Γ^v₁₅．在这种方法里，可以考虑反演不对称性、能带的非抛物性、有效质量不连续性以及自旋轨道耦合等效应的影响．作为应用，计算了两个量子阱结构的子带和光跃迁概率．实验上在这两个结构中观察到了平面内极化的电子子带跃迁．计算表明这种跃迁的概率很小．实验上观察到的平面内极化的电子子带吸收可能有其他的机制 关键词：     

类氦离子Cr^22＋精细结构能级和光谱跃迁的相对论多组态 …

采用相对论多组态自洽场方法,计算了Ｃｒ＾２２＋离子的精细结构能级,能级宽度,激发态寿命和光谱跃迁参数。计算中考虑了核的有限体积效应,Ｂｒｅｉｔ修正,ＱＣＤ修正和轨道极化效应。所得结果与文献的实验值和计算值进行了比较。     

铬的电离势及类氦Cr22+的E2和M1光谱跃迁的全相对论计算

基于相对论多组态自洽场方法,计算了CrⅠ至CrⅩⅩⅣ 离子的基态能量和各价电离势,类氦Cr22+离子的电四极矩和磁偶极矩光谱跃迁数据 。计算中考虑了核的有限体积效应、Berit修正、QED修正和轨道极化效应。计算结果与文献 的实验和计算值进行了比较。     

激光晶体MgO:Ni2+的DV-Xx研究

本文将我们提出的一种在DV-Xα计算过渡金属络合物电子结构的基础上计算光谱的方法用于激光晶体MgO:Ni2+的研究.首次从第一性原理出发,全面计算了该激光晶体的单电子能谱、总态密度、自旋极化分裂、电荷转移跃迁能量、特别是d-d跃迁多重光谱项能量和自旋一轨道耦合常数,得到了与实验值较一致的结果.     

The design of a polarizing beam splitter made from a dielectric rectangular-groove grating

It has been reported that a polarizing beam splitter based on a rectangular-groove grating (a grating polarizing beam splitter) can be easily designed for specific applications using the modal method. In this paper, the eigenvalue equation of the modal method is transformed to a new form. Using this new form of the eigenvalue equation, it is shown that the design of a grating polarizing beam splitter can be independent of the incident wavelength. The period and the groove depth can be designed using values normalized to the incident wavelength, which apply to a range of wavelengths as long as the effects of dispersion can be neglected. Numerical simulations of fused silica gratings are presented and analyzed. It is concluded that the preferable choice for the grating period is 0.8–0.9 times the incident wavelength.     

Laser cavities and polarization optics for soft X-rays and the extreme ultraviolet

Addressed here are polarization optics for extreme-ultraviolet and soft X-ray wavelengths, especially as relevant to laser cavities. It is pointed out that the whisper-gallery mirrors studied by Vinogradov can serve as weak polarizers and, more importantly, as birefringent elements. The application of multilayer technology to polarizing mirrors and beamsplitters is also considered. It is shown that multilayer beamsplitters can function both as reflective and transmissive polarizers. Their behavior is surprising in some cases, with the same polarization being preferred in both reflection and transmission. Three polarizing cavity schemes are proposed, each incorporating a polarizing beamsplitter as its output coupler. Cavity optimization issues are discussed.     

Two orthogonal polarized wavelengths generated in a N2-laser pumped dye laser

Outputs at two wavelengths with orthogonal polarizations are generated in a N₂-laser pumped dye laser by a simple method. The light leaving the laser cavity at the side exit of the polarizing Glan-Thompson is redirected into the cavity via an additional mirror and a second Glan-Thompson. Depending on its polarization light is travelling different paths and may hit the grating at different angles. In this way feedback is produced for two separate light beams and lasing can take place at two wavelengths simultaneously.     

Fabrication Techniques and Characteristics of Ultra-Thin Optical Polarizing Films Using Gold Island Films

Fabrication techniques of ultra-thin optical polarizing films using gold island films have been investigated for the near-infrared region. The polarizing films are fabricated by stretching the periodic multilayers consisting of gold island layers and glass layers. We have experimentally investigated the optimum fabricating conditions necessary to induce large optical anisotropy into the gold island layers and have formed submicrometer-thick polarizing films with an extinction ratio of ≥20 dB in a near-infrared region longer than 800 nm. These polarizing films could be useful micro-polarizers for fiber-embedded in-line optical devices, micro-optics, and hybrid integrated optics.     

Fabrication and Patterning of Submierometer-Thick Optical Polarizing Films for 800 nm Using Stretched Silver Island Multilayers

Stretched silver island multilayers have been investigated for patterned optical polarizers for the wavelength of 800 nm. Submicrometer-thick optical polarizing films are fabricated by stretching periodic multilayers consisting of silver island layers and Pyrex layers at the temperature of 660°C. As the optical anisotropy of the optical polarizing film is lost by heating at a temperature higher than the stretching temperature, the fine non-polarizing areas can be deliberately and easily formed on the optical polarizing film by laser irradiation with high power density. We have successfully formed various non-polarizing areas on the optical polarizing film with a 1 W-class carbon dioxide laser. The demonstrated fabricating techniques of deliberately patterned optical polarizing films should be useful for novel optical computing and sensing devices.     

水窗波段反射式偏振光学元件的设计和制作

水窗波段是软X射线进行生物活细胞显微成像的最佳波段,因此对于水窗波段偏振光学元件的研究有着非常重要的意义。用菲涅耳公式计算出在水窗波段内不同材料组合对应不同波长的最大反射率,模拟分析了多层膜周期和表界面粗糙度对多层膜偏振光学元件性能的影响。用超高真空磁控溅射镀膜设备,制作出2．40nm、3．00nm和4．30nm波长处W／B4C多层膜偏振元件,并用X射线衍射仪对元件的周期厚度进行了测量,得到的测量结果与设计值偏差很小,可以进行实际应用。为水窗波段反射式偏振光学元件的研究提供了理论依据,同时也为相应偏振光学元件的制备确定了合适的工艺参量。     

Effect of UV radiation on the optical and some structural properties of irregular rayon acetate fibers

This recent study shed demonstration on how the structural parameters changes due exposure to UV radiation and different wavelengths. So this article throws light on the changes of the optical properties and some structural properties due exposure to UV radiation and different wavelengths on irregular rayon acetate fibers. Pluta polarizing interference microscope is used to study the changes for refractive indices and birefringence with different exposure times at three different intensities on irregular rayon acetate fibers. As the principal optical parameters determined, these give an indication of the isotropic refractive index, stress optical coefficient, stress due to UV radiation, optical configuration parameter, segment anisotropy, the number of molecules per unit volume and polarizability of a monomer unit can be obtained. Also by using different wavelengths are given the spectral dispersions, Cauchy's dispersion constants, the resonant wavelength, the oscillation energy, the dispersion energy, the dielectric constant and the dielectric susceptibility for rayon acetate fibers with different wavelengths at room temperatures. Illustrations are given using graphs and microinterferograms.     

Experimental determination of optical constants of MgF2 and AlF3 thin films in the vacuum ultra-violet wavelength region (60-124 nm), and its application to optical designs

The investigation of some solar radiations of interest for astrophysicists requires optics in the 80-130 nm vacuum ultra-violet spectral range (VUV). In this domain, where both transmittance and reflectance of most materials are very low, the measurement of optical constants is specifically difficult, and optical data are consequently often either inexistent or uncertain. Reliable modelling of optical components for VUV, like polarizing multi-layered mirrors, necessitates prior measurement of complex indices of the thin films involved in the coating. Fluorides like MgF₂ or AlF₃ are among the rare materials capable to contribute to multi-layer mirrors in the VUV.We have determined optical constants of thin films of these two materials by using a two media reflectance method at normal incidence and a graphical determination particularly suited to this VUV region, which we presented in a previous paper. Optical constants are determined in the range 60-124 nm with 2 nm step, and are compared to existing data. On the basis of these measured indices, polarizing mirrors for λ₁ = 121.6 nm or λ₂ = 103.2 nm have been modelled and fabricated. Their reflectance measured versus incidence angle by using monochromatized synchrotron radiation at the above wavelengths is found in agreement with the calculated predictions.     

Compound polarized wavelength filters with a single subwavelength structure

A novel dual functional device that combines functions of polarizing and bandpass filtering together using a single subwavelength structure is proposed. Characteristics of both wavelength filtering and polarizing in the visible wavelength range with two different multi-layer subwavelength structures are investigated. It is found that both filtering and polarizing functions can be realized simultaneously by appropriate design of the substrate, a dielectric layer and a metallic layer system. Dependence of tunable filtering central wavelength on the properties of layered materials and structural dimensions are discussed in detail. Typical optimized multilayer structural parameters are obtained, in which ~ 75% passband transmission with > 30 dB polarization extinction ratio have been achieved simultaneously for three primary color (red, green and blue) filters. The results open new possibilities in designing and fabricating novel multi-functional polarizing and filtering photonic devices using a single subwavelength structure.     

The photoinduced polarization in Kapton-H film

The photoinduced polarization in Kapton-H thin film has been studied by analysing the isothermal dark decay characteristics of photo- and dark-polarized specimens for different values of the polarizing parameters. The total polarization induced has been found to increase continuously with polarizing temperature but with polarizing field, it approaches a saturation. The behaviour of dark decay currents for photo and dark polarized identical samples changes with operating temperature. The phenomenon is explained in terms of the shift of electrons and hole demarcation levels under variation of temperature and illumination intensity.on study leave from S.G.R.R. (P.G.) College, Dehradun, India