气相Lys分子体系捕获双电子单重激发态的特性

采用密度泛函理论（DFT）中的B3LYP方法, 在6-311+G(2df)基组水平上, 对气相赖氨酸（Lys）分子和Lys^2-的基态稳定构型进行优化, 并用含时密度泛函理论（TD DFT)方法考察气相Lys分子和带电离子体系单重激发态的特性. 结果表明： Lys分子体系捕获双电子时, 其体系能量有所增加； S1单重激发态与S0基态能量差值变小； 分子体系的荧光波长增加； S7单重激发态跃迁轨道数减少.     

一维周期和非周期体系的电子带谱及态密度

本文发展了一种重正化群方法,精确而系统地研究包含周期和非周期格子的一维体系的物理性质.该一体系的构造序列是选A、B两块并按膨胀规则{A、B}→{A~(m11)B~(m12),A~(m12)B~(m22)}排列成的.作为特例,计算了(M_(11),M_(12),M_(21),M_(22))=(1,1,1,0)(1,1,1,1)(1,2,1,1)和(2,1,1,1)几种一维格子的电子带谱和态密度,结果表明,较之其他方法,该方法具有系统性,而且分析结果与其他类似。     

顺式丁二烯及其一氟、一氯取代物电环化反应过程的量子化学研究

用密度泛函理论（DFT）的B3LYP方法在6－311＋＋G**基组水平上研究了cis-1,3-丁二烯及其一氟、一氯取代物电环化反应过程的微观机理，优化得到了反应途径上的反应物、过渡态和产物的几何构型，通过振动分析对过渡态进行了确认，并对优化得到的单点在QCISD（T）水平上计算了能量。研究结果表明：cis-1,3－丁二烯的氟、氯代衍生物各有两种构象，且均能发生环化反应，两种构象环化的产物是一致的；亚甲基上外侧的氢原子被氟、氯原子取代后，有利于环化反应的进行。     

篮球运动员赛前心理准备与调节

赛前心理训练是篮球运动员必备的专业素质之一，它的作用在于挖掘心理潜力、发挥心理优势，使运动员的身体素质、技术水平和心理水平在比赛中达到最佳竞技状态，只有这样，运动员才能临阵不慌，在激烈的角逐中获得主动．     

用于分布式识别的语音参数的提取和性能分析

主要研究用于分布式语音识别(DSR)的语音参数的提取方法以及参数性能分析。以前所用到的语音参数大部分是LPC倒谱参数,但其抗噪声性能较差。文中主要讨论了MEL倒谱参数,并在移动通信环境下,比较了两者的性能。     

类He离子双电子S激发态的描述

在含有电子相互关系的薛定谔方程近似解的基础上，建立类Ｈｅ等电子离子双激发Ｓ态的能量与核电荷及量子数的依赖关系，并导出一能对高激发态能量进行定量分析的近似公式。     

The v-v energy transfer of highly vibrationally excited states (I)

The relaxation of the highly vibrationally excited CO (v = 1–8) by CO₂ is studied by timeresolved Fourier transform infrared emission spectroscopy (TR FTIR). 193 nm laser photolysis of the mixture of CHBr₃ with O₂ generates the highly vibrationally excited CO(v) molecules. TR FTIR records the intense infrared emission of CO(v→v-1). The vibrational populations of each level of CO(v) have been determined by the method of spectral simulation. Based on the evolution of the time resolved populations and the differential method, 8 energy transfer rate constants of CO(v = 1–8) to CO₂ molecules areobtained: (5.7±0.1), (5.9±0.1), (5.2±0.2), (3.4±0.2), (2.4±0.3), (2.2±0.4), (2.0±0.4) and (1.8±0.6) (10¹⁴ cm³ · molecule⁻¹ · s⁻¹), respectively. A two-channel energy transfer model can explain the feature of the quenching of CO(v) by CO². For the lower vibrational states of CO, the vibrational energy transfers preferentially to the u³ mode of CO² For the higher levels, the major quenching channel changes to the vibrational energy exchange between CO(v→v-1) and the u¹ mode of CO².     

The v-v energy transfer of highly vibrationally excited states (II)

The vibrational energy transfer from highly vibrationally excited CO to H₂O molecules is studied by time-resolved Fourier transform infrared emission spectroscopy (TR FTIR). Following the 193 nm laser photolysis of CHBr₃ and O₂ the secondary reactions generate CO(v). The infrared emission of CO(v → v−1) is detected by TR FTIR. The excitation of H₂O molecules is not observed. By the method of the spectral simulation and the differential technique, 8 rate constants for CO(v)/H₂O system are obtained: (1.7 ±0.1), (3.4 ±0.2), (6.2 ±0.4), (8.0 ±1.0), (9.0 ±2.0), (12 ±3), (16 ±4) and (18 ±7) (10¹³cm³ · molecule^-1· s^-1). At least two reasons lead to the efficient energy transfer. One is the contributions of the rotational energy to the vibational energy defect and the other is the result of the complex collision. With the SSH andab initio calculations, the quenching mechanism of CO(v) by H₂O is suggested.