NeNO分子光谱常数和非谐振力场的算法研究

本论文分别用从头算方法（B3LYP、MP2）结合基组cc-pVNZ (N ∈ {T,D,Q}) 及 6-311G、6-311G（2df,2pd）计算了NeNO分子的平衡几何结构、光谱常数和非谐振力场.结果表明：在MP2方法下计算的结果略优于B3LYP计算的结果;基组6-311G、6-311G（2df,2pd）下的结果相对优于cc-PVNZ (N=T,D,Q)得到的结果;MP2理论方法结合基组6-311G、6-311G（2df,2pd）基组计算的结果非常接近实验值,这些计算结果对实验测量某些光谱数据有较好的预测作用.     

ArNO分子光谱常数和非谐振力场的理论研究

本论文分别用从头算方法（B3LYP、B3PW91、MP2）结合基组（aug）cc-pVNZ（N∈{T,D,Q}）及6-311G、6-311G^**、6-311G（2df,2pd）、6-311G（3df,3pd）计算了ArNO分子的平衡几何结构、光谱常数和非谐振力场.结果表明:在MP2方法下计算的结果要优于B3LYP和B3PW91计算的结果;基组6-311G、6-311G^**、6-311G（2df,2pd）、6-311G（3df,3pd）下的结果普遍优于cc-PVNZ（N=T,D,Q）得到的结果;MP2理论方法结合基组6-311G、6-311G^**、6-311G（2dr,2pd）、6-311G（3df,3pd）基组计算的结果非常接近实验值,对实验测量某些光谱数据有较好的预测作用.     

HeNO分子光谱常数和非谐振力场的从头算研究

在本论文中,我们在Gaussian 03软件下,采用密度泛函理论（B3LYP）以及二阶微扰理论（MP2）的方法结合Dunning相关一致基组cc-pVNZ (N=T,D,Q)以及6-311G、6-311G**、6-311G（2df,2pd）、6-311G（3df,3pd）基组优化了HeNO分子的几何结构,然后在此基础上计算了它们的光谱常数和非谐振力场。通过计算得到了分子的平衡几何结构、基频、转动常数、四次和六次离心畸变常数等,并与相关的实验值和理论值进行了比较;预测了部分光谱常数,其中包括谐振频率、非谐性常数、振转相互作用常数、三次力常数、四次力常数和科里奥利耦合常数。结果表明,在MP2方法下计算的结果要优于B3LYP计算的结果;基组6-311G、6-311G**、6-311G（2df,2pd）、6-311G（3df,3pd）下的结果普遍优于cc-PVNZ (N=T,D,Q)得到的结果。结果还表明,MP2理论方法结合基组6-311G、6-311G**、6-311G（2df,2pd）、6-311G（3df,3pd）基组计算的结果非常接近实验值,对实验测量某些光谱数据有较好的预测作用     

HeNO分子光谱常数和非谐振力场的从头算研究

本文利用Gaussian 03软件,采用密度泛函理论(B3LYP)以及二阶微扰理论(MP2)的方法结合Dunning相关一致基组cc-pVNZ (N=T,D,Q)以及6-311G、6-311G**、6-311G(2df,2pd)、6-311G(3df,3pd)基组优化了HeNO分子的几何结构,然后在此基础上计算了它们的光谱常数和非谐振力场.通过计算得到了分子的平衡几何结构、基频、转动常数、四次和六次离心畸变常数等,并与相关的实验值和理论值进行了比较;预测了部分光谱常数,其中包括谐振频率、非谐性常数、振转相互作用常数、三次力常数、四次力常数和科里奥利耦合常数.结果表明,在MP2方法下计算的结果要优于B3LYP计算的结果;基组6-311G、6-311G**、6-311G(2df,2pd)、6-311G(3df,3pd)下的结果普遍优于cc-PVNZ (N=T,D,Q)得到的结果.结果还表明,MP2理论方法结合基组6-311G、6-311G**、6-311G(2df,2pd)、6-311G(3df,3pd)基组计算的结果非常接近实验值,对实验测量某些光谱数据有较好的预测作用.     

NeNO分子光谱常数和非谐振力场的从头算研究

本文用从头算方法(B3LYP、MP2)计算了NeNO分子的光谱常数和非谐振力场.结果表明:在MP2方法下采用基组6-311G、6-311G(2df,2pd)计算的结果相对于实验和前人计算的结果优于B3LYP方法下采用基组cc-PVNZ(N=T,D,Q)计算的结果;重要的是这些计算结果对实验测量某些光谱数据(平衡转动常数、非谐常数等)有一定的预测作用.     

HNCS分子的光谱常数和非谐振力场的理论研究

采用Gaussian09数据包,以密度泛函理论（B3LYP、B3PW91）和二阶微扰（MP2）方法,分别采用基组6-311+G、6-311++G(2d,2p)、cc-PVNZ(N=T,Q)以及加入弥散函数的高角动量基组aug-cc-PVNZ(N=T,Q)等计算了HNCS分子的光谱常数和非谐振力场。结果表明：B3LYP、B3PW91和MP2计算的结果与实验结果都比较接近;当基组由VTZ增大到VQZ或加弥散函数对结果的影响均不明显;其中B3PW91\cc-PVTZ的各项计算结果相对于其他计算结果更接近实验值。通过计算,可以在前人基础上进一步预测HNCS分子其它的光谱常数（如:非谐性常数、科里奥利耦合常数等）。     

CaS基态（ ）结构及势能函数研究

采用B3LYP、BP86、B3P86、QCISD、CCSD方法.分别选用6-311G(2df,3pd)、6-311G(2df,2pd)、6-311G(3df,2pd)、6-311G(3df,3pd)、sddall、sdd基组对CaS基态（ ）分子进行结构优化.最后选用最佳基组B3LYP/6-311G(3df,3pd)的计算结果.分别对Murrell- Sorbie（i=3,4,5,6,7,8,9）函数及修正的函数Murrell- Sorbie+ 运用最小二乘法拟合运算,导出CaS分子的力常数（ ）;最终选用最能反映CaS性质的函数Murrell- Sorbie（i=9）,计算CaS光谱常数（ ）.结果表明：用Murrell- Sorbie（i=9）函数计算出的 比选用Murrell- Sorbie（i=3,4,5,6,7,8）及Murrell- Sorbie+ 更接近实验数据;用Murrell- Sorbie（i=9）计算的CaS分子光谱常数与理论值非常吻合;CaS分子运用 Murrell- Sorbie（i=9）函数能够准确表达.     

HNCS分子的光谱常数和非谐振力场的理论研究

采用Gaussian09数据包,以密度泛函理论(B3LYP、B3PW91)和二阶微扰(MP2)方法,分别采用基组6-311+G、6-311++G(2d,2p)、cc-PVNZ(N=T,Q)以及加入弥散函数的高角动量基组aug-ccPVNZ(N=T,Q)等计算了异磺氰酸(HNCS)分子的光谱常数和非谐振力场.结果表明:B3LYP、B3PW91和MP2计算的结果与实验结果都比较接近;当基组由VTZ增大到VQZ或加弥散函数对结果的影响均不明显;其中B3PW91/cc-PVTZ的各项计算结果相对于其他计算结果更接近实验值.通过计算,可以在前人基础上进一步预测HNCS分子其它的光谱常数(如:非谐性常数、科里奥利耦合常数等).     

CaS基态(X~1∑~+)结构及势能函数研究

采用B3LYP、BP86、B3P86、QCISD、CCSD方法.分别选用6-311G（2df,3pd）、6-311G（2df,2pd）、6-311G（3df,2pd）、6-311G（3df,3pd）、sddall、sdd基组对CaS基态（X¹∑⁺）分子进行结构优化.最后选用最佳基组B3LYP/6-311G（3df,3pd）的计算结果.分别对Murrell-Sorbie（i=3,4,5,6,7,8,9）函数及修正的函数Murrell-Sorbie+G₆运用最小二乘法拟合运算,导出CaS分子的力常数（f₂,f₃,f₄）;最终选用最能反映CaS性质的函数Murrell-Sorbie（i=9）,计算CaS光谱常数（ω_e,B_e,α_e,ω_eχ_e）.结果表明:用MurrellSorbie（i=9）函数计算出的f₂,f₃,f₄比选用Murrell-Sorbie（i=3,4,5,6,7,8）及Murrell-Sorbie+C₆更接近实验数据;用Murrell-Sorbie（i=9）计算的CaS分子光谱常数与理论值非常吻合;CaS分子运用MurrellSorbie（i=9）函数能够准确表达.     

MgH分子X2Σ+,A2Π和B2Σ+电子态的势能函数

利用QCISD(T),SAC-CI方法和cc-pVQZ,aug-cc-pVTZ,6-311 G及6-311 G(3df,2pd)基组,对MgH分子的基态X2Σ ,第一简并激发态A2Π和第二激发态B2Σ 的结构进行优化计算.通过对4个基组计算结果进行比较,得出6-311 G(3df,2pd)基组为最优基组.使用6-311 G(3df,2pd)基组和QCISD(T)方法对基态X2Σ ,SAC-CI方法对激发态A2Π和B2Σ 进行单点能扫描计算,然后采用Murrell-Sorbie函数及修正的Murrell-Sorbie C6函数进行拟合,得到了相应电子态的势能函数参数和对应的光谱常数.计算结果表明,用修正的Murrell-Sorbie C6函数计算得到的MgH分子基态和第一简并激发态的光谱常数ωe,ωexe,Be,αe与实验数据吻合很好.表明修正后的Murrell-Sorbie C6函数能更为准确地描述MgH分子的基态和第一激发态的势能函数.     

Guided-Wave Two-Dimensional Acousto-Optic Scanner Using Proton-Exchanged Lithium Niobate Waveguide

Two-dimensional scanning of a 0.6328 mum guided-light beam has been realized using noncolinear acousto-optic (AO) coplanar Bragg diffraction together with colinear AO guided-mode to substrate radiation-mode conversion in a Z-cut Xpropagation LiNbO3 proton-exchanged (PE) waveguide. The two surface acoustic (SAW) waves utilized are at the center frequencies of 500 and 200 MHz, propagating in the Y and X axes, respectively. Two-dimensional scanning of approximately 720 resolvable light beam spots, namely, 18 40 (horizontal vertical) scanning, has been demonstrated using a light beam of 1.0 mm aperture. The total number of resolvable beam spots can be greatly increased from 720 by simply utilizing SAW transducers of larger bandwidth and a light beam of greater aperture. It should also be possible to significantly increase the diffraction efficiency from 3 % by optimizing the parameters of the PE waveguide and the SAWs.     

Femtosecond Transform-Limited Pulse Generation by Compensating for the Linear Chirp of SPM Spectra in Dispersion Shifted Fibers

A simple technique of pulse compression, based on the linear chirp compensation of self-phase modulation (SPM) spectra in dispersion shifted fibers, is demonstrated. The optimization procedure is carried out, for a short span of a single-mode fiber, using a parabolic law, which describes the behavior of the squared output pulse width versus the pump peak power in the case of Gaussian pulses. The experimental results give a minimum pulse duration of 233 fs, which is in good agreement with the model. Shorter and coherent pulses, down to 90 fs, have been obtained by inserting an interference filter at the optical output.     

Effect ofγ-radiation on the spectral luminescence characteristics of impure cadmium tungstate crystals

Results of a study of the effect of γ-radiation on the spectral luminescence properties of cadmium tungstate crystals doped with silver, bismuth, and molybdenum cations are presented. Spectral characteristics of the nondnnnoped crystals are briefly described. Absorption and photo and X-ray luminescence spectra of the crystals taken before and after exposure to γ-radiation (5.5·10⁴ Gy) are compared. It is found that the spectral characteristics of the crystals doped with silver, bismuth, and molybdenum cations do not change markedly after the exposure. The relation between the type of impurity-induced defects, individual characteristics of the impurity cations, and the character of the effect of γ-radiation on the spectral luminescence properties of impure crystals is analyzed (preliminarily). Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 64, No. 1, pp. 55–60, January–February, 1997.     

Theoretical analysis and simulation of conjugate heights for dual-conjugate AO system in lidar

A multi-conjugate adaptive optics （MCAO） can offer a possibility of widening field of view （FOV） characterized by the isoplanatic angle, and the choose of conjugate height becomes a basic problem for MCAO, which influences the size of iosplanatic angle. Considering the application of lidar, the isoplanatic angle＇s expressions of two deformable mirrors （DMs） MCAO for uplink and downlink are deduced. The effects of conjugate heights for dual-conjugate AO are thoughtfully discussed, and the isoplanatic angles are further analyzed. The results show that the isopanatic angle varies with the conjugate height and reaches the maximum as the conjugate height is at the optimal altitude. Moreover, the optimal conjugate height changes with the propagation distance.     

Quick single-photon detector with many avalanche photo diodes working on the time division

Due to the limit of response speed of the present single-photon detector, the code rate is still too low to come into practical use for the present quantum key distribution (QKD) system.A new idea is put up to design a quick single-photon detector.This quick single-photon detector is composed of a multi-port optic-fiber splitter and many avalanche photo diodes (APDs).Au of the ports with APDs work on the time division and cooperate with a logic discriminating and deciding unit driven by the clock signal.The operation frequency lies on the number N of ports, and can reach N times of the conventional single-photon detector.The single-photon prompt detection can come true for high repetition-rate pulses.The applying of this detector will largely raise the code rate of the QKD, and boost the commercial use.     

Sorting of bending magnets for the SSRF booster

The Shanghai Synchrotron Radiation Facility(SSRF)booster ring,a full energy injector for the storage ring,is deigned to accelerate the electron beam energy from 150MeV to 3.5GeV that demands high extraction efficiency at the extraction energy with low beam loss rate when electrons are ramping.Closed orbit distortion(COD)caused by bending magnet field uniformity errors which affects the machine performance harmfully could be effectively reduced by bending magnet location sorting.Considering the affections of random errors in measurement,both ideal sorting and realistic sorting are studied based on measured bending magnet field uniformity errors and one reasonable combination of bending magnets which can reduce the horizontal COD by a factor of 5is given as the final installation sequence of the booster bending magnets in this paper.     

Improvement of four-wave mixing-based wavelength conversion efficiency in dispersion shifted fiber by 40-GHz clock pumping

40-GHz clock modulated signal as a pump to improve the efficiency of four-wave mixing (FWM)-based wavelength conversion in a 26.5-km dispersion shifted fiber (DSF) is investigated. The experimental results demonstrate that the conjugated FWM component has higher intensity with the clock pumping than that with the continuous-wave (CW) light pumping. The improvement of FWM-based wavelength conversion efficiency is negligible when the pump power is less than Brillouin threshold. But when the pump power is greater than Brillouin threshold, the improvement becomes significant and increases with the increment of pump power. The improvement can increase up to 9 dB if pump power reaches 17 dBm.     

Characterization of PolyA and PolyC mismatches by Raman spectroscopy

A.C mismatches are studied by Raman spectral characterization of PolyA, PolyC, and their equimolar complex in solution of 0.14 mol/L Na ,pH7.0.Experimental results show that A·C mismatches occur to be A/B (mainly A) conformers, and unlike Watson-Crick base pairing, this kind of mismatches is stabilized by only one hydrogen bond involving cytosine N4H2 and adenine N7.The formation of A·C complex makes the base stacking interactions much stronger, and conformation of the backbone more ordered, which leads to obvious Raman hypochromic effect with some shifts in corresponding bands.