Λ-related Quantum Interference of 2∏[Case(a)] Diatom on Rotational Energy Transfer

为了从理论上研究碰撞转动传能量子干涉中积分干涉角与散射角之间的关系,在洪德a情况下提出了原子-双原子分子体系积分干涉角．在一级波恩近似的基础上,考虑了长程相互作用势,提出了双原子分子Λ分裂2∏态洪德a情况下碰撞诱导转动传能的理论模型．在洪德a情况下讨论了干涉程度,并定量地计算了CN(A2∏)在洪德a情况下与碰撞伴He、Ne和Ar的碰撞诱导转动传能的干涉角,进而得到了与积分干涉角有关的各个参量．     

Electron localization in ultrathin films of three-dimensional topological insulators

The recent discovery of three-dimensional(3D) topological insulators(TIs) has provided a fertile ground for obtaining further insights into electron localization in condensed matter systems.In the past few years,a tremendous amount of research effort has been devoted to investigate electron transport properties of 3D TIs and their low dimensional structures in a wide range of disorder strength,covering transport regimes from weak antilocalization to strong localization.The knowledge gained from these studies not only offers sensitive means to probe the surface states of 3D TIs but also forms a basis for exploring novel topological phases.In this article,we briefly review the main experimental progress in the study of the localization in 3D TIs,with a focus on the latest results on ultrathin TI films.Some new transport data will also be presented in order to complement those reported previously in the literature.     

理论研究强激光场中2pz态氢原子的电离

运用强场近似速度规范理论研究了激发态氢原子的电离情况,当 a.u. 时（ω是激光场的频率,γ是Keldysh绝热参数）,在线性极化激光场中推导了2pz态氢原子电离率的简单表达式,从公式中可以看出在低频极限的情况下,电离率和激光场频率ω成正比,这一公式对激发态氢原子电离机制的研究提供了重要的理论参考。     

亚锗基卡宾及取代亚锗基卡宾与环氧乙烷抽提反应机理的密度泛函理论研究

采用B3LYP/6-311G(d,p)方法研究了单重态亚锗基卡宾及取代亚锗基卡宾X₂Ge=C:(X=H, F, Cl, CH₃)与环氧乙烷的氧转移反应机理. 结果表明, 由于环氧乙烷中氧上的2p孤对电子向X₂Ge=C:中C上的2p空轨道迁移,形成了p→p授受键,从而生成了各中间体. 随着p→p授受键的不断加强(即C-O键的逐渐缩短),中间体经过渡态生成了抽提产物. 取代基的电负性是影响该类反应的主要因素,取代基的电负性越大,反应的活化能越小     

1Π态双原子分子中关于(A)量子干涉的微分干涉角

Sha等在静态池实验中观察到了转动能量转移中的碰撞量子干涉,并且计算了决定跃迁散射截面的积分干涉角(J.Chem.Phys.,1995,102:2772).由于积分干涉角是微分干涉角的平均效应,为了得到更精确的信息,进行了分子束实验.作者文运用含时微扰的一级波恩近似理论,提出了衡量干涉程度的1П态双原子分子中关于Λ量子干涉的微分干涉角.利用各向异性相互作用势计算了其干涉角.得到分子束实验中微分干涉角随实验参数,包括实验温度、碰撞伴、作用距离和转动量子数变化的关系.并且讨论了影响干涉角的各种参数.此理论模型对理解和进行分子束实验是非常重要的.     

^1Π态双原子分子中关于∧量子干涉的微分干涉角

Sha等在静态池实验中观察到了转动能量转移中的碰撞量子干涉,并且计算了决定跃迁散射截面的积分干涉角（J.Chem.Phys.,1995,102：2772）.由于积分干涉角是微分干涉角的平均效应,为了得到更精确的信息,进行了分子束实验.作者文运用含时微扰的一级波恩近似理论,提出了衡量干涉程度的^1П态双原子分子中关于Λ量子干涉的微分干涉角.利用各向异性相互作用势计算了其干涉角.得到分子束实验中微分干涉角随实验参数,包括实验温度、碰撞伴、作用距离和转动量子数变化的关系.并且讨论了影响干涉角的各种参数.此理论模型对理解和进行分子束实验是非常重要的.     

2-(N,N-二乙基苯胺-4-基)-4,6-双(3,5-二甲基比唑-1-基)-1,3,5三嗪的电子结构和光物理性质

采用量子化学计算方法研究了2-(N,N-二乙基苯胺-4-基)-4,6-双(3,5-二甲基吡唑-1-基)-1,3,5三嗪(dpbt)聚合物的电子结构和光物理性质，并且用二维实空间和三维实空间分析方法进行理论研究．结果表明, dpbt聚合物的第一激发态为分子内电荷转移激发态，存在较大的电偶极距变化和极化率，其中电偶极距变化与实验数值符合较好，理论计算所得到极化率数值与实验结果一致．S1激发态存在较大的电偶极距变化和极化率会导致非线性光学效应，促使高效的双光子吸收截面的形成．同时对外电场变化时dpbt的激发态性质进行理论研究．     

近共振电子态和转动能量传递AB(1∑,J)+C(slj)→AB(1∑,J'')+C(slj'')

1995年沙等在静态池实验中观测到了碰撞诱导转动传能中的量子干涉效应,并且测量到了决定跃迁截面幅值的积分干涉角(J.Chem.Phys.,1995,102,2772).同时,孙等在理论上计算了CO A1Ⅱ(v=0)～e3∑-(v=1)与He,Ne以及其它碰撞伴的碰撞体系的积分干涉角,建立了相应的理论模型.然而,以前的研究都局限在碰撞伴通常被认为是没有结构的粒子,但是在碰撞过程中相互碰撞的两个粒都有内部角动量,自旋-轨道相互作用又对反应速率起着非常重要的影响,同时也能够影响反应势垒的高度,因此这种近似忽略了碰撞伴原子对整个碰撞体系得影响.基于这种考虑,在这篇文章中我们从理论上研究AB (1∑,J)+C(slj)→AB(1∑,J')+C(slj')的碰撞诱导的电子态和转动态的能量传递,应用一级含时波恩近似、各向异性L-J相互作用势和直线轨迹近似,建立了理论模型.并讨论和比较了在近共振电子态和非共振电子态两种情况下的振动传能的跃迁几率.     

Excited state intramolecular proton transfer mechanism of o-hydroxynaphthyl phenanthroimidazole

By utilizing the density functional theory(DFT) and the time-dependent density functional theory(TDDFT), the excited state intramolecular proton transfer(ESIPT) mechanism of o-hydroxynaphthyl phenanthroimidazole(HNPI) is studied in detail. Upon photo is excited, the intramolecular hydrogen bond is obviously enhanced in the S_1 state, which thus promotes the ESIPT process. Hydrogen bond is shown to be strengthened via comparing the molecular structures and the infrared vibration spectra of the S_0 and S_1 states. Through analyzing the frontier molecular orbitals, we can conclude that the excitation is a type of the intramolecular charge transfer excitation, which also indicates the trend of proton transfer in S_1 state. The vertical excitation based on TDDFT calculation can effectively repeat the absorption and fluorescence spectra of the experiment. However, the fluorescence spectrum of normal structure, which is similar to the spectrum of isomer structure is not detected in the experiment. It can be concluded that the fluorescence measured in the experiment is attributed to both structures. In addition, by analyzing the potential energy curves(PECs) calculated by the B3 LYP functional method, it can be derived that since the molecule to cross the potential barrier in the S_1 state is smaller than in the S_0 state and the reverse proton transfer process in the S_1 state is more difficult than in the S_0 state, the ESIPT occurs in the S_1 state.     

4氢-吡喃-4-硫酮~1(n→π*),~1A_g~-(π→π*)和~1B_u~+(π→π*)等的激发态特征(英文)

理论上4氢-吡喃-4-硫酮的激发态特征用量子化学方法以及二维实空间分析法和三维立体实空间分析法加以研究.理论上的结果揭示^1（n→π^＊）和^1Ag^-（π→π^＊）激发态是分子内电荷转移（ICT）激发态,而^1Bu^＋（π→π^＊）激发态是离域激发态.它们的跃迁偶极矩的强度和方向用三维密度跃迁（TD）加以解释,用三维电荷密度差（CDD）观察分子间电荷转移（ICT）的激发态特征或局部激发态特征.用二维实空间分析法研究电子-空穴相关性,离域化和激子的尺寸.