振动激发对O+DCl→OD+Cl反应动力学性质的影响

采用准经典轨线方法讨论了反应物分子的振动激发对O+DCl→OD+Cl反应动力学性质的影响.计算结果表明,反应物分子的振动激发对(2π/σ)(dσ00/dωt),(2π/σ)(dσ20/dωt)和(2π/σ)(dσ22+/dωt)3个极化微分反应截面和产物分子转动角动量取向程度的影响比较显著.变化规律反映出反应物分子的高振动激发使产物分子倾向于在平行于散射面的平面内转动.     

气相中原子分子成簇动力学Ⅰ.动力学的基本模型

提出了气相原子、分子碰撞形成团簇的动力学一般模型，认为具有特定组份单元的粒子经碰撞后可任意组合成团簇．各缔合速率常数随团簇的尺寸和结构特征而变化．团簇的热解离速率主要取决于断键数．因此裂解出小碎片的几率较大．将上述模型用动力学方程表示，可计算在不同时刻的团簇尺寸分布．最后分析了激光烧蚀、电弧放电等几种形成团簇方法的具体条件．     

Ag/Se二元团簇的形成以及Ag与Se团簇反应的研究

用飞行时间质谱仪研究了激光直接溅射Ag/Se混合样品产生的二元团簇以及团簇正离子的光解行为;并用串级溅射反应装置研究了Ag和Se正负离子产物.在直接溅射产生的Ag/Se二元团簇中,正离子主要系列是:[(Ag₂Se)_nAg⁺],[(Ag₂Se)_nAg₃⁺];负离子主要系列是:[(Ag₂Se)_nAgSe^-],[(Ag₂Se)_nAgSe₂^-],[(Ag₂Se)_nSe^-].团簇正离子的光解结果表明,同样条件下Ag/Se二元团簇正离子光解比率比Ag/S大.在Ag和Se样品串级溅射实验中,主要得到AgSe_n⁺(n=4～9)和AgSe_nSe^-(n=4～7)系列的产物,在AgSe_n⁺系列中,n=4,6时丰度较大.这表明串级溅射反应和直接溅射二元混合样品两种过程中成簇机理是不同的.     

气相中原子分子成簇动力学 I. 动力学的基本模型

提出了气相原子，分子碰撞形成团簇的动力学一般模型，认为具有特定组分份单元的粒子经碰撞后可任意组合成团簇，各缔合速率常数随团簇的尺寸和结构特征而变化，团簇的热解离速率主要取决于断键数，因此裂解出小碎片的几率较大，将上述模型用动力学方程表示，可计算在不同时刻的团簇尺寸分布，最后分析了激光烧蚀，电弧放电等几种形成团簇的方法的具体条件。     

反应Si+HCl→SiCl+H的直接动力学研究

利用从头算直接动力学方法，研究反应Si HCl→SiCl H的动力学性能，在QCISD／6－311＋G（d,p)和CCSD（T）／aug-cc-pvtz(单点）水平上，得到体系的势能面信息，进而利用变分过渡态理论计算了反应的速率常数及其与温度的关系。计算结果与实验符合得很好。     

钴原子团簇用于高效氧还原反应

探索非贵金属材料作为高效氧还原反应催化剂是迫切需要的,但具有一定的挑战性。本文采用等离子体轰击和酸洗相结合的策略合成了Co原子团簇修饰的多孔碳载体催化剂(Co_AC/NC)。通过多种表征手段证实了的原子团簇特征。所得到的Co_AC/NC催化剂在三电极体系和锌-空电池方面都表现出优异的氧还原反应活性。该催化剂的氧还原反应半波电位为0.887 V,显著优于商业Pt/C催化剂,且表现出优异的稳定性。此外,该催化剂组装的锌-空电池的峰值功率密度为181.5 mW∙cm⁻²,同样远高于Pt/C催化剂。这项工作不仅合成了一种高效的氧还原反应催化剂,而且为原子团簇催化剂的理性设计和实际应用提供了新的见解。     

激光溅射下原子团簇生长的非平衡动力学(I)

以激光溅射的方式,可以产生不同尺寸与组分的原子团簇.但是对这些团簇的生长过程,却一直缺少比较深入和细致的研究.本文结合激光真空溅射石墨的实验条件,考虑了激光能量、体系膨胀、环境压力、热量辐射等诸多因素,建立了在该条件下碳原子团簇生长的物理模型,得出了相应的动力学方程的数值解.计算结果表明:每个激光脉冲溅射出约8×10-9mol(5×1015个)粒子,它们产生时的初始压力约为2×105Pa.由于扩散等因素,团簇的形成反应在7.85μs后已不可能进行,但是各团簇产物的产率在反应开始后0.4μs左右已达到最大值,在约1.5μs内反应即已基本完成,因为此后原子团簇的尺寸分布不再有显著的差异.     

激光溅射下原子团簇生长的非平衡动力学

以激光溅射的方式,可以产生不同尺寸与组分的原子团簇．但是对这些团簇的生长过程,却一直缺少比较深入和细致的研究．本文结合激光真空溅射石墨的实验条件,考虑了激光能量、体系膨胀、环境压力、热量辐射等诸多因素,建立了在该条件下碳原子团簇生长的物理模型,得出了相应的动力学方程的数值解．计算结果表明：每个激光脉冲溅射出约8×10－9mol（5×1015个）粒子,它们产生时的初始压力约为2×105Pa．由于扩散等因素,团簇的形成反应在785μs后已不可能进行,但是各团簇产物的产率在反应开始后0．4μs左右已达到最大值,在约1．5μs内反应即已基本完成,因为此后原子团簇的尺寸分布不再有显著的差异．     

D+HCN反应的SVRT含时波包理论研究

基于Horst的势能面,用SVRT(SemirigidVibratingRotorTarget)方法对D+HCN反应进行了含时波包动力学研究,计算得到了不同初始振转态的总反应几率和积分反应截面,采用UniformJ-shifting方法得到该反应的热速率常数.计算结果与H+HCN反应进行了比和讨论.     

反应N+NH→N2+H的态-态量子动力学研究

采用在MRCI/aug-cc-pVQZ水平上构建的N₂H基态势能面, 并运用Chebyshev实波包法研究了N + NH→N₂ + H反应的量子动力学, 如反应几率、 积分截面以及产物振转态分布等. 在50~500 K温度范围内, 该反应的速率常数随着温度升高而递增, 与基于其它势能面的理论结果吻合. 然而, 在室温条件下, 所有理论计算的速率常数均显著大于实验值.     

State to State Photodissociation Dynamics of Vibrationally Excited D2O in B Band

The state-to-state photodissociassion dynamics for the B band of D₂O have been explored from quantum dynamical calculations including the electronic ~X and ~B states. The calculations were carried out using a Chebyshev real wave packet method. The calculated absorption spectra, product state distributions, and branching ratios from different initial vibrational states show di?erent dynamic features, due to the different shapes of the vibrational wavefunctions. The initial bending mode (0,1,0) generates two lobes with a shallow minimum on the absorption spectrum and a slight inverted vibrational population of OD(~X )product at high total energies. The rotational state distributions of OD(~X , v=0) product are highly inverted and depend weakly on the initial state and total energy. On the other hand, the ro-vibrational distributions of OD(A~) product strongly oscillate with the total energy, which are dominated by the long-living resonances and depend sensitively on the potential surfaces. The antisymmetric stretching mode (0,0,1) has large OD( ~ A)/OD(~X ) branching ratios at high total energies, which indicates that the B band dissociation proceeds mainly via the adiabatic pathway in some cases.     

4-硝基咪唑A-带激发态结构动力学

通过共振拉曼光谱实验和量子化学计算的方法研究了4-硝基咪唑(4NI)A-带激发态衰变动力学. 对4NI的振动光谱、紫外电子吸收光谱、荧光光谱和共振拉曼光谱进行了指认. 在全活化空间自洽场法(CASSCF)/6-31G(d)计算水平下获得了单重激发态S₁(n_Oπ^*)和S₂(ππ^*)和势能面交叉点S₁(n_Oπ^*)/S₂(ππ^*)的优化几何结构和能量, 分析了A-带共振拉曼光谱的强度模式特征, 获得了短时结构动力学, 并结合全活化空间自洽场法(CASSCF)理论计算结果确定了4NI 在S₂(ππ^*)态衰变通道主要是S_{2, FC}→S_{2, min}(ππ^*)→S₀辐射弛豫.     

4-硝基咪唑A-带激发态结构动力学

通过共振拉曼光谱实验和量子化学计算的方法研究了4-硝基咪唑(4NI)A-带激发态衰变动力学.对4NI的振动光谱、紫外电子吸收光谱、荧光光谱和共振拉曼光谱进行了指认.在全活化空间自洽场法(CASSCF)/6-31G(d)计算水平下获得了单重激发态S1(nOπ*)和S2(ππ*)和势能面交叉点S1(nOπ*)/S2(ππ*)的优化几何结构和能量,分析了A-带共振拉曼光谱的强度模式特征,获得了短时结构动力学,并结合全活化空间自洽场法(CASSCF)理论计算结果确定了4NI在S2(ππ*)态衰变通道主要是S2,FC→S2,min(ππ*)→S0辐射弛豫.     

Micro-Solvated DMABN: Excited State Quantum Dynamics and Dual Fluorescence Spectra

In this work, we report a complete analysis by theoretical and spectroscopic methods of the short-time behaviour of 4-(dimethylamino)benzonitrile (DMABN) in the gas phase as well as in cyclohexane, tetrahydrofuran, acetonitrile, and water solution, after excitation to the La state. The spectroscopic properties of DMABN were investigated experimentally using UV absorption and fluorescence emission spectroscopy. The computational study was developed at different electronic structure levels and using the Polarisable Continuum Model (PCM) and explicit solvent molecules to reproduce the solvent environment. Additionally, excited state quantum dynamics simulations in the diabatic picture using the direct dynamics variational multiconfigurational Gaussian (DD-vMCG) method were performed, the largest quantum dynamics “on-the-fly” simulations performed with this method until now. The comparison with fully converged multilayer multiconfigurational time-dependent Hartree (ML-MCTDH) dynamics on parametrised linear vibronic coupling (LVC) potentials show very similar population decays and evolution of the nuclear wavepacket. The ring C=C stretching and three methyl tilting modes are identified as the responsible motions for the internal conversion from the La to the Lb states. No major differences are observed in the ultrafast initial decay in different solvents, but we show that this effect depends strongly on the level of electronic structure used.     

丙烯酸分子的激发态超快预解离动力学

利用飞秒泵浦-探测技术结合飞行时间质谱(TOF-MS),研究了丙烯酸分子被200nm泵浦光激发到第二电子激发态(S2)后的超快预解离动力学.采集了母体离子和碎片离子的时间分辨质谱信号,并利用动力学方程对时间分辨离子质谱信号进行拟合和分析,揭示了预解离通道的存在.布居在S2激发态的分子通过快速的内转换弛豫到第一电子激发态(S1),时间常数为210fs,随后再经内转换从S1态弛豫到基态(S0)的高振动态,时间常数为1.49ps.分子最终在基态高振动态势能面上发生C-C键和C-O键的断裂,分别解离生成H2C=CH和HOCO、H2C=CHCO和OH中性碎片,对应的预解离时间常数分别约为4和3ps.碎片离子的产生有两个途径,分别来自于母体离子的解离和基态高振动态势能面上中性碎片的电离.     

Excited State Dynamics of Isolated 6- and 8-Hydroxyquinoline Molecules

The photoinduced dynamics of isolated n-hydroxyquinoline (nHQ) molecules (n=6,8) was investigated in femtosecond pump-probe experiments. A qualitative difference was found between 8HQ and 6HQ. After an initial rapid decay corresponding to the departure of the initial wavepacket out of the Franck-Condon region of the excitation, the 8HQ probe signal decays to zero in 0.37 ps whereas a much longer time constant of 10.4 ps is observed in 6HQ. This interrogates on the role played by the intramolecular H-bond N HO which is at play the 8HQ molecule. Ab-initio were performed at the MCSCF/aug-cc-pVDZ level on the 8HQ molecule to help the discussion. A complex energy landscape was found, which includes a conical intersection.     

Classical Reactive Molecular Dynamics Implementations: State of the Art

Reactive molecular dynamics (RMD) implementations equipped with force field approaches to simulate both the time evolution as well as chemical reactions of a broad class of materials are reviewed herein. We subdivide the RMD approaches developed during the last decade as well as older ones already reviewed in 1995 by Srivastava and Garrison and in 2000 by Brenner into two classes. The methods in the first RMD class rely on the use of a reaction cutoff distance and employ a sudden transition from the educts to the products. Due to their simplicity these methods are well suited to generate equilibrated atomistic or material‐specific coarse‐grained polymer structures. In connection with generic models they offer useful qualitative insight into polymerization reactions. The methods in the second RMD class are based on empirical reactive force fields and implement a smooth and continuous transition from the educts to the products. In this RMD class, the reactive potentials are based on many‐body or bond‐order force fields as well as on empirical standard force fields, such as CHARMM, AMBER or MM3 that are modified to become reactive. The aim with the more sophisticated implementations of the second RMD class is the investigation of the reaction kinetics and mechanisms as well as the evaluation of transition state geometries. Pure or hybrid ab initio, density functional, semi‐empirical, molecular mechanics, and Monte Carlo methods for which no time evolution of the chemical systems is achieved are excluded from the present review. So are molecular dynamics techniques coupled with quantum chemical methods for the treatment of the reactive regions, such as Car–Parinello molecular dynamics.     

Si2分子基态和低激发态的电子结构

本文用abinitioSOCI／MCSCF／／HF／DH＋d方法计算得到了Si2分子的基态和八个激发态的平衡几何构型、总能量、谐振动频率、零点能以及各个态的势能曲线．讨论了各态键长随电子组态的变化关系，指出了成健轨道中。电子数的增加，是引起键长及谐振动频率变化的重要因素·其中3Πg，5∑；3△u，3∑，未见有关文献报导由于硅藻合物的重要应用价值，人们已对其进行了一些实验和理论研究h，’」．以前的研究主要是讨论其成键性质．由于St。分子结构的特殊性，要想全面了解其成键性质，不仅要研究其基态的电子结构，而且还要研究其激发态的电…     

离子液体[Bmim][BF_4]中卟啉的三线态动力学

室温离子液体由于其几乎不挥发、稳定性突出、良好的电化学性能以及结构与性能的可设计性等优点,在诸多领域得到了深入的研究和广泛的应用。与传统的普通溶剂不同,离子液体的本质特点之一是其内部的微观结构具有微不均匀性。本文通过对四苯基卟啉(TPP)分子在离子液体[Bmim][BF_4]中的三线态动力学研究,发现在激光作用下,TPP的三线态寿命由2.95μs显著增加到184μs。进一步分析表明,这一现象很可能是由于离子液体的微结构在激光诱导下发生变化,被激光场或者离子诱导极化的氧气分子在离子液体微不均匀性环境中发生重新分布而引起的。     

Ultrafast Decay Dynamics of 2-Hydroxypyridine Excited to S1 Electronic State

The S\begin{document}$_1$\end{document} state decay dynamics of 2-hydroxypyridine following UV excitation at a wavelength range of 276.9\begin{document}$-$\end{document}250.0 nm is investigated using femtosecond time-resolved photoelectron imaging technique. Based on pump wavelength dependence of the decay dynamics, a refined decay picture is proposed. At pump wavelength of 276.9 nm, the S\begin{document}$_1$\end{document} state is depopulated through intersystem crossing to lower triplet state(s). At 264.0 nm, both intersystem crossing to lower triplet state(s) and internal conversion to the ground state are in operation. At 250.0 nm, internal conversion to the ground state becomes dominated.