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1.
采用密度泛函理论B3LYP 方法研究了CF2 自由基与HNCO 的反应机理, 并在B3LYP/6-311++G**水平上对反应物、中间体、过渡态进行了全几何参数优化, 通过频率分析和内禀反应坐标(IRC)确定了中间体和过渡态.为了得到更精确的能量值, 又用CCSD(T)/6-311++G**方法计算了在B3LYP/6-311++G**水平优化后的各个驻点的相对能量. 根据统计热力学及用Winger校正的Eyring过渡态理论,利用自编程序,计算不同温度下低势垒反应的平衡常数和速率常数.计算结果表明单重态的CF2 自由基与HNCO 的反应有四条反应通道, 三重态的CF2 自由基与HNCO 的反应有两条反应通道.其中单重态反应通道CF2+HNCO→1IM1→1TS1→1IM2→1TS2→1IM3→CF2NH+CO(P1)为主反应通道.三重态反应通道CF2+HNCO→36IM1→36TS1→36IM2→HCF2+NCO(3P5)为主反应通道.  相似文献   

2.
采用密度泛函理论B3LYP 方法研究了CF2 自由基与HNCO 的反应机理, 并在B3LYP/6-311++G**水平上对反应物、中间体、过渡态进行了全几何参数优化, 通过频率分析和内禀反应坐标(IRC)确定了中间体和过渡态.为了得到更精确的能量值, 又用CCSD(T)/6-311++G**方法计算了在B3LYP/6-311++G**水平优化后的各个驻点的相对能量. 根据统计热力学及用Winger校正的Eyring过渡态理论,利用自编程序,计算不同温度下低势垒反应的平衡常数和速率常数.计算结果表明单重态的CF2 自由基与HNCO 的反应有四条反应通道, 三重态的CF2 自由基与HNCO 的反应有两条反应通道.其中单重态反应通道CF2+HNCO→1IM1→1TS1→1IM2→1TS2→1IM3→CF2NH+CO(P1)为主反应通道.三重态反应通道CF2+HNCO→36IM1→36TS1→36IM2→HCF2+NCO(3P5)为主反应通道.  相似文献   

3.
采用密度泛函理论B3LYP 方法研究了CF2 自由基与HNCS 的反应机理, 并在B3LYP/6-311++G**水平上对反应物、中间体、过渡态进行了全几何参数优化. 为了得到更精确的能量值,又用CCSD(T)/6-311++G**方法计算了在B3LYP/6-311++G**水平优化后的各个驻点的相对能量. 根据统计热力学及用Winger校正的Eyring过渡态理论,利用自编程序,计算不同温度下低势垒反应的平衡常数和速率常数.计算结果表明单重态的CF2 自由基与HNCS 的反应有6条反应通道,三重态的CF2 自由基与HNCS 的反应有1条反应通道.其中单重态反应通道CF2+HNCS→IM1→TS1→IM2 HCF2NCS(P1)为主反应通道.  相似文献   

4.
应用密度泛函理论对 ClF3 O 和环氧丙烷的反应机理进行了研究。在 B3PW91/6-31++G(d ,p )水平上优化了各驻点(反应物、中间体、过渡态和产物)的几何构型,并计算了它们的振动频率和零点振动能。采用 CCSD(T)/6-31++G(d ,p )//B3PW91/6-3l++G(d ,p )单点能计算方法求得各物质的能量,并做零点能校正。计算结果表明,ClF3 O 与 C3 H 6 O 可经过不同的反应路径,引发 C3 H 5 O 自由基和 ClOF2自由基生成环氧丙醇和三氟化氯,其中,位于 ClF3 O 周向位置的 F 原子与 C3 H 6 O 的 C(7)上与 CH 3异侧的 H(9)原子结合的活化能最低,仅15.63 kJ/mo1;ClF3 O 与 C3 H 6 O 反应生成的 C3 H 5 O 自由基和 ClOF2自由基继续反应,经过不同反应路径生成 C3 H 4 O、ClOF 和 HF,其中,ClOF2中的 F 原子和 C3 H 5 O 中的 H(2)或 H(4)原子结合是无能垒的过程。整个反应的主要路径为 C3 H 6 O+ClF3→O→TS12 P4(C3 H 5 O+HF+ClOF2→) P12(CH 2 CHCHO+2 HF+ClOF)。  相似文献   

5.
应用密度泛函理论对ClF3O和环氧丙烷的反应机理进行了研究。在B3PW91/6-31++G(d,p)水平上优化了各驻点(反应物、中间体、过渡态和产物)的几何构型,并计算了它们的振动频率和零点振动能。采用CCSD(T)/6-31++G(d,p)//B3PW91/6-3l++G(d,p)单点能计算方法求得各物质的能量,并做零点能校正。计算结果表明,ClF3O与C3H6O可经过不同的反应路径,引发C3H5O自由基和ClOF2自由基生成环氧丙醇和三氟化氯,其中,位于ClF3O周向位置的F原子与C3H6O的C(7)上与CH3异侧的H(9)原子结合的活化能最低,仅15.63kJ/mo1;ClF3O与C3H6O反应生成的C3H5O自由基和ClOF2自由基继续反应,经过不同反应路径生成C3H4O、ClOF和HF,其中,ClOF2中的F原子和C3H5O中的H(2)或H(4)原子结合是无能垒的过程。整个反应的主要路径为C3H6O+ClF3O→TS12→P4(C3H5O+HF+ClOF2)→P12(CH2CHCHO+2HF+ClOF)。  相似文献   

6.
应用量子理论从头算和密度泛函理论(DFT)对双自由基CH(X2Π)与O2(X3∑g-)的反应机理进行了研究.在B3PW91/6-311G**水平上优化了反应通道上各驻点(反应物、中间体、过渡态和产物)的几何构型,并计算了零点能和过渡态的虚频率.并由B3PW91/6-311G**给出了各物种的总能量.计算表明,反应物中自由基CH与O2反应主要在二重态势能面上进行,CH中的C原子可以插在O2分子中两个氧原子中间形成中间体1(2HCO2),中间体1(2HCO2)可以经过不同的反应通道形成不同的产物P1(1CO2 2H)和P2(1CO 2OH),各反应通道的反应热的计算与实验值吻合较好.  相似文献   

7.
采用密度泛函理论B3LYP方法研究了CF2自由基与HNCS的反应机理,并在B3LYP/6-311++G**水平上对反应物、中间体、过渡态进行了全几何参数优化,通过频率分析和IRC确定中间体和过渡态的真实性.为了得到更精确的能量值,又用CCSD(T)/6-311++G**方法计算了在B3LYP/6-311++G**水平优化后的各个驻点的相对能量.根据统计热力学及用Winger校正的Eyring过渡态理论,利用自编程序,计算不同温度下低势垒反应的平衡常数和速率常数.计算结果表明,单重态的CF2自由基与HNCS的反应有6条可能的反应通道,三重态的CF2自由基与HNCS的反应有1条反应通道.其中单重态反应通道CF2+HNCS→IM1→TS1→IM2 HCF2NCS(P1)为主反应通道.  相似文献   

8.
采用密度泛函理论B3LYP方法研究了CF_2自由基与HNCO的反应机理,并在B3LYP/6-311++G**水平上对反应物、中间体、过渡态进行了全几何参数优化.为了得到更精确的能量值,又用CCSD(T)/6-311++G**方法计算了在B3LYP/6-311++G**水平优化后的各个驻点的相对能量.根据统计热力学及用Winger校正的Eyring过渡态理论,利用自编程序,计算不同温度下低势垒反应的平衡常数和速率常数.计算结果表明单重态的CF_2自由基与HNCO的反应有四条反应通道,三重态的CF_2自由基与HNCO的反应有两条反应通道.其中单重态反应通道CF_2+HNCO→1IM1→1TS1→1IM2→1TS2→1IM3→CF_2NH+CO(P1)为主反应通道.三重态反应通道CF_2+HNCO→~36IM1→~36TS1→~36IM2→HCF_2+NCO(~3P5)为主反应通道.  相似文献   

9.
4-氟苯甲醛酪氨酸席夫碱(4-FT)由4-氟苯甲醛和L-酪氨酸钾盐在室温条件下反应制得,4-FT的结构通过1HNMR,FTIR和Raman测试得到确认。分别用密度泛函(DFT,density functional theory)理论的B3LYP(Becke’s three-parameter exchange functional(B3)with Lee,Yang,Parr(LYP))方法和从头算(ab initio)理论的HF(Hartree-Fock)方法,选用标准的6-31G**和6-31G*基组对化合物4-FT的几何构型进行优化。同时分别在B3LYP/6-31G**,B3LYP/6-31G*,HF/6-31G**和HF/6-31G*水平下计算4-FT的振动波数。用密度泛函(DFT)的B3LYP方法计算并校正后的波长数据比用从头算(ab i-nitio)的HF方法计算的结果更与实验数据吻合。  相似文献   

10.
采用密度泛函理论B3LYP方法研究了CCl2自由基与HNCO的反应机理,并在B3LYP/6-311++G**水平上对反应物,中间体,过渡态进行了全几何参数优化,通过频率分析和IRC确定中间体和过渡态。为了得到更精确的能量值,用QCISD(T)/6-311++G**方法计算了各个驻点的单点能,计算结果表明单重态的二氯卡宾与异氰酸的反应有抽提氧、插入N-H键、抽提亚氨基的路径。而插入通道HNCO + CCl2→IM3 →TS2→P2(C2Cl2ONH) 反应能垒最低, 为主反应通道。  相似文献   

11.
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.  相似文献   

12.
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.  相似文献   

13.
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.  相似文献   

14.
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.  相似文献   

15.
16.
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.  相似文献   

17.
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.  相似文献   

18.
19.
We measure the waveform and phase curves of short optical pulses before and after transmission over different lengths of fibers by use of the pulse analyzer with the frequency-resolved optical gating (FROG),and numerically simulate pulse evolution under the experimental conditions.The nonlinear coefficient of the fiber is given by comparing the experimental results with the numerical ones.Difference between the experiment and numerical simulation is analyzed.  相似文献   

20.
Resonance scattering of elastic spherical shell and cylindrical shell while the surrounding fluid medium has absorption is studied. The normal mode solution derived using exact elastic theory and the separation of variables is still applicable. However, the scattering form function has to be modified for the absorbing medium, otherwise the unreasonable result would be obtained. The backscattering form function in the absorbing medium is redefined, and the form function of elastic spherical and cylindrical shell with vacuum or solid matter filled is calculated in various absorption conditions. The results show that the absorption of surrounding fluid leads to notable attenuation of the coincidence resonances in the mid-frequency, but it has a little influence on the low-frequency resonance scattering induced by the filler inside the shell.  相似文献   

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