[Ar…Ar-H]+分子振动光谱的理论计算

中心对称的线性结构[Ar-H-Ar]M⁺及非对称线性结构[Ar…Ar-H]⁺是[Ar₂H]⁺的两个稳定构型. 基于近期由本组提供的[Ar₂H]⁺分子的基态势能面, 应用含时波包演化方法计算了总角动量J = 0时的[Ar…Ar-H]SUP>+构型下的振动光谱, 观察到量子隧道效应对振动光谱的影响, 并通过观察本征态波函数性质以及修饰势能面等方法对其中的一些谱峰进行了指认, 发现[Ar-H-Ar]⁺构型的高弯曲振动激发态与[Ar…Ar-H]⁺的振动态之间存在强烈耦合的现象.     

铁原子与氮分子间的相互作用——单端位构型

用杂化密度泛函B3LYP方法在6-311+G(d)基组水平上研究了Fe 原子与N2分子相互作用的单端位构型的直线形和弯曲形两种结构的平衡几何结构、电子结构、轨道布局及红外光谱等性质. 计算结果表明, 由于强的σ-σ电子对互斥作用, 基组态4s²3d⁶的Fe原子不能与N2分子发生化学作用; 当Fe 原子呈现可与N2之间发生σ-π授予反馈作用的激发组态时, Fe 与N2分子之间可形成稳定的结构; 在得到的多个电子态中, 能量最低的是直线形的1³∑^-, 比Fe(a⁵D)和N2(¹∑⁺g )能量高21.6 kJ·mol-1, 同时存在几个能量相近的电子态, 如1³∏、1³Φ; 弯曲形都是不稳定态, 可能是连接直线形和单侧双配位构型的过渡态; 单端位构型产物相对于基态的反应物均是热力学不稳定的; 单端位构型中Fe对N2的活化作用很小, N—N 键长增加不超过7 pm.     

乙烯自由基A2A''(v'=0)←X2A'(v''=0)带的转动分析

通过193 nm光解丁烯酮分子产生乙烯基自由基(C₂H₃). 经射流冷却后, 用另一束激光光解C₂H₃, 生成的氢原子碎片经共振增强多光子电离(REMPI)过程, 记录氢离子信号随光解波长变化, 得到20020～20070 cm_-1范围内乙烯基激发的转动分辨光谱. 该谱对应于A²A'(v'=0)←X²A'(v'=0)跃迁的转动结构. 结合量子化学理论计算、光谱拟合以及前人的研究结果, 对该段光谱进行了完整的转动识别, 确定了40条转动谱线的位置. 由光谱拟合还得到A²A'(v'= 0 )能级的预解离寿命为3.3 ps, 且不依赖于转动量子数.     

Cl2+2HBr=2HCl+Br2反应的机理和应用

用密度泛函理论(DFT)B3LYP方法,取6-311G**基组,细致研究了反应Cl2+2HBr= 2HCl+Br2的机理,求得一系列四中心和三中心过渡态.双分子基元反应Cl₂+HBr®HCl+ BrCl和BrCl+HBr®Br₂+HCl的活化能(138.96和147.24 kJ· mol-1)小于Cl₂,HBr和BrCl的解离能,从理论上证明了标题反应将优先以分子与分子作用形式完成.将其应用于从HBr中回收溴,以Cl₂直接与HBr气体反应,生成的含溴混合气体,经冷凝并以四氯化碳吸收分离得到液溴和盐酸;溴的回收率大于96%,其含氯量小于3.0%.提供了运用基础理论解决生产中难题的成功例证.     

(BCO)+n(n=1-12)团簇的结构与稳定性

用密度泛函理论(DFT)的B3LYP方法, 在6-31G*水平上对(BCO)⁺_n(n=1-12)团簇的几何结构、电子结构、振动频率等性质进行了理论研究. 结果表明, (BCO)⁺_n团簇的基态结构均为羰基端配位(μ₁-CO)结构, 且含三元环和五元环数目越多或四元环和六元环的数目越少, 相应的结构越稳定. 能量分析得到, n 为奇数的(BCO)⁺_n团簇比n为偶数的稳定.     

含铁杂多酸盐MÖssbauer谱研究 Ⅱ.铁钼硅杂多蓝中Fe的状态和反磁性交换

制备了铁钼硅杂多蓝阴离子[SiFe^ⅢMo^ⅤMo₁₀^ⅥO₄₀H₃]^5-的钾盐和四丁铵盐,应用⁵⁷Fe同位素增丰法测定了匹丁铵盐的Mossbauer谱。结合磁化率测定和红外光谱数据,研究了杂多蓝阴离子中铁的价态和自旋态等,推测由于Mo-O-Fe之间氧桥的作用,相邻金属原子上的d电子之间存在反磁性交换。实验结果肯定了这一推测。     

Cl2+2HI=2HCl+I2反应机理的理论研究

分别在MP2/3-21G**、CCSD(T)/3-21G**//MP2/3-21G**和B3LYP/3-21G**3种水平上, 计算研究了气相反应Cl₂+2HI=2HCl+I₂的机理, 求得一系列四中心和三中心的过渡态. 通过比较六种反应通道的活化能大小, 得到了相同的结论：双分子基元反应Cl₂+HIHCl+ICl和ICl+HII₂+HCl的最小活化能小于Cl₂、HI和ICl的解离能, 从理论上证明了反应Cl₂+2HI=2HCl+I₂将优先以分子与分子作用形式分两步完成. 用内禀反应坐标(IRC)验证了MP2/3-21G**方法计算得到的过渡态.     

甲基萘醌光敏化单电子氧化多聚鸟苷酸的动态研究

用248 nm激光光解瞬态吸收光谱研究了乙腈-水混合溶液中甲基萘醌(MQ)激发三重态(3MQ^*)单电子氧化多聚鸟苷酸(polyG)的原初过程, 应用解析瞬态吸收谱方法分别获取了MQ阴离子自由基(MQ^-·)及polyG阳离子自由基(polyG^+·)的瞬态吸收谱, 进而分别测定了MQ^-·及polyG^+·的生成速率常数及3MQ^*的衰减速率常数. 结果表明, 3MQ^*与polyG的反应速率常数非常接近于3MQ^*与dGMP反应的速率常数.     

氯代(对位取代四苯基)卟啉铁(Ⅲ)的轴向配位反应热力学及光谱研究

本文对二氯甲烷溶剂中咪唑(Im)与氯代(对位取代四苯基)卟啉铁(Ⅲ)[Fe(p-X)TPPCl,X=Cl,H,CH₃,OCH₃]的轴向配位反应(1)进行了研究.用光谱法测得了反应(1)的平衡常数,并对反应物和产Fe(p-X)TPPCl+2Im⇔[Fe(p-X)TPPIm₂]⁺Cl^-物的电子光谱、FeHTPPCl和[FeHTPPIm₂]⁺Cl^-的电子自旋共振谱和穆斯堡尔谱进行了测量.研究了取代基效应和轴向配体的影响.     

[Si,N,N,P]体系异构体结构与稳定性

在B3LYP/6-311G(d)和QCISD(t)/6-311+G(2df)(单点)水平下计算得到了[Si,N,N,P]体系势能面上的一些驻点, 研究了异构体之间的异构化过程, 并讨论了该体系异构体的结构与稳定性. 结果表明在[Si,N,N,P]体系中的11个异构体中只有含有Si-P交叉成键的类蝶型四元环异构体SiNPN(E1, ²A″)是稳定的, 其他异构体由于易于重排或是解离, 稳定性较低. 研究同时给出了E1的电子与几何结构、振动频率及指认、偶极矩和转动常数等相关数据. 分析结果表明通过中间体E3(SiNPN)的反应SiN(²Π) + PN(¹Σ)→E1是由SiN(²Π)和PN(¹Σ)碎片产生E1的最有利途径, 因此E1可成为星际观测的目标. G2级别下此反应的反应焓变为215.25 kJ/mol (298.15 K), 而异构体E1在298.15 K下的标准生成焓为457.99 kJ/mol.     

Two-photon dissociation spectroscopy of state-selected HCl+ and DCl+ ions.

HCl+ and DCl+ ions were formed via the R(1) pump line of the f3delta2(v'=0)<--sigma+(v'=0) REMPI process. For these ions, the two-photon dissociation spectroscopy, resonance-enhanced via the A2sigma+(v')<--pi3/2(v'=0) transition, was investigated for various intermediate states of HCl+ (v'=4,5,6) and DCl+ (v'=6,7,8,9). From the analysis of the data, spectroscopic parameters of the X and the A states were derived (including the lambda-doubling in the X state and the spin-rotation coupling in the A state). Some of the parameters deviate considerably from literature data. The spectra provide clear evidence that the REMPI process employed for forming the ions has a very high rotational selectivity.     

Photoelectron imaging following 2 + 1 multiphoton excitation of HBr

The photodissociation and photoionization dynamics of HBr via low-n Rydberg and ion-pair states was studied by using 2 + 1 REMPI spectroscopy and velocity map imaging of photoelectrons. Two-photon excitation at about 9.4-10 eV was used to prepare rotationally selected excited states. Following absorption of the third photon the unperturbed F (1)Delta(2) and i (3)Delta(2) states ionize directly into the ground vibrational state of the molecular ion according to the Franck-Condon principle and upon preservation of the ion core. In case of the V (1)Sigma(+)(0(+)) ion-pair state and the perturbed E (1)Sigma(+)(0(+)), g (3)Sigma(-)(0(+)), and H (1)Sigma(+)(0(+)) Rydberg states the absorption of the third photon additionally results in a long vibrational progression of HBr(+) in the X (2)Pi state as well as formation of electronically excited atomic photofragments. The vibrational excitation of the molecular ion is explained by autoionization of repulsive superexcited states into the ground state of the molecular ion. In contrast to HCl, the perturbed Rydberg states of HBr show strong participation of the direct ionization process, with ionic core preservation.     

Photofragmentations, state interactions, and energetics of Rydberg and ion-pair states: two-dimensional resonance enhanced multiphoton ionization of HBr via singlet-, triplet-, Ω = 0 and 2 states

Mass spectra were recorded for one-colour resonance enhanced multiphoton ionization (REMPI) of H(i)Br (i = 79, 81) for the two-photon resonance excitation region 79,040-80,300 cm(-1) to obtain two-dimensional REMPI data. The data were analysed in terms of rotational line positions, intensities, and line-widths. Quantitative analysis of the data relevant to near-resonance interactions between the F(1)Δ(2)(v' = 1) and V(1)Σ(+)(v' = m + 7) states gives interaction strengths, fractional state mixing, and parameters relevant to dissociation of the F state. Qualitative analysis further reveals the nature of state interactions between ion-pair states and the E(1)Σ(+) (v' = 1) and H(1)Σ(+)(v' = 0) Rydberg states in terms of relative strengths and J' dependences. Large variety in line-widths, depending on electronic states and J' quantum numbers, is indicative of number of different predissociation channels. The relationship between line-widths, line-shifts, and signal intensities reveals dissociation mechanisms involving ion-pair to Rydberg state interactions prior to direct or indirect predissociations of Rydberg states. Quantum interference effects are found to be important. Moreover, observed bromine atom (2 + 1) REMPI signals support the importance of Rydberg state predissociation channels. A band system, not previously observed in REMPI, was observed and assigned to the k(3)Π(0)(v' = 0) ←← X transition with band origin 80,038 cm(-1) and rotational parameter B(v('))=7.238 cm(-1).     

The dissociation dynamics of He...I 35Cl(B,v'=2,3) complexes with varying amounts of internal energy

The He...I (35)Cl intermolecular vibrational levels with n'=0-6 that are bound within the He+ICl(B,v'=3) potential [A. B. McCoy, J. P. Darr, D. S. Boucher, P. R. Winter, M. D. Bradke, and R. A. Loomis, J. Chem. Phys. 120, 2677 (2004)] are identified in laser-induced fluorescence experiments performed at very low temperatures within a supersonic expansion. Comparisons of the positions and intensities of these lines with the excitation spectra, calculated using potential surfaces to describe the interactions between the helium atom and ICl in its ground and excited state, assist in the assignments. Based on these comparisons the excited state potential was rescaled so that the experimental and calculated J'=0 energies agree to within the experimental uncertainties for all but the lowest, n'=0, intermolecular level. Two-laser, action, and pump-probe spectroscopy experiments indicate that the bound He...I (35)Cl(B,v'=3) intermolecular vibrational levels undergo vibrational predissociation forming rotationally excited I (35)Cl(B,v'=2,j') products with distributions that depend upon the initial intermolecular vibrational level excited. Action spectra recorded in the ICl B-X, 2-0 region while monitoring the Deltav=0, I (35)Cl(B,v'=2) channel reveal two additional dissociation mechanisms for the He...I (35)Cl(B,v') excited state complexes: rotational predissociation of discrete metastable states lying slightly above the He+I (35)Cl(B,v'=2) asymptote and direct dissociation that occurs when the linear conformer is excited to the continuum of states above the same asymptote. The rotational predissociation pathway forms I (35)Cl(B,v'=2,j') products in all of the rotational states energetically accessible. The direct dissociation mechanism yields very cold rotational product state distributions; for instance, the average rotational energy in the product state distribution measured when the linear complexes are prepared 20 cm(-1) above the dissociation limit is only 1.51 cm(-1), representing only 7.6% of the available energy.     

N2O+离子B2П态的光谱与光解离动力学

用一束波长为360.55 nm的激光直接作用于超声射流的N₂O分子束, 通过(3+1)共振增强多光子电离(REMPI)过程制备纯净的N₂O⁺(X²П(0,0,0))母体离子, 再用另一束波长在243-278 nm范围的激光将母体离子激发至B²П态后解离. 扫描解离激光波长, 监测NO⁺离子碎片的强度, 从而获得N₂O⁺离子B²П态的光致碎片激发(PHOFEX)谱. 通过拟合转动分辨光谱, 得到了相应的转动常数和自旋分裂常数, 从而区分了A²Σ⁺态高振动能级和B²П态带源的贡献, 明确了N₂O⁺离子B²П态的光谱"带头"位置(37154 cm^-1), 并将获得的振动光谱初步归属为B²П(v₁,v₂,v₃)←X²П的振动跃迁序列. 通过对NO⁺碎片离子的飞行时间质谱峰形的分析, 还获得了解离过程中释放的平均平动能, 并结合电子激发态势能面, 讨论了N₂O⁺离子B²П态的解离机理.     

Unravelling the reactivity of antisymmetric stretch-excited CH4 with Cl by-product pair-correlation measurements

The vibrational branching ratio [CH(3)(v=0) + HCl(v'=1)]/[CH(3)(v=0) + HCl(v'=0)] of two correlated product pairs from the title reaction shows a dramatic E(c)-dependence, in sharp contrast to the previously observed behavior in Cl + CHD(3)(v(1)=1), while the vibrational enhancement factors in reactivity of the two reactions are remarkably similar.     

Vibrational relaxation dynamics of I35Cl(B, v') induced by low-temperature collisions with He atoms

Using laser-induced fluorescence and two-laser, pump-probe spectroscopy, collision-induced vibrational relaxation is observed to compete with the dissociation of electronically excited ICl in a helium carrier gas expansion. By thoroughly characterizing the expansion properties, we observe that collisions of ICl(B, v'= 3) molecules with He atoms in the expansion induce vibrational relaxation of the initially prepared dihalogen down to rotor states in the next lower ICl(B,v'= 2) level on timescales that compete with the rate for non-adiabatic transfer from the B state to the Z1 state. The resulting ICl(B,v'= 2,j') product rotational distribution, along with the analogous ICl(B,v'= 1,j') distribution formed by collisional relaxation of molecules in the long-lived ICl(B,v'= 2) level are compared to ICl(B,v'= 2,j') products formed by vibrational predissociation of He...ICl complexes prepared in different intermolecular vibrational levels within the He + ICl(B,v'= 3) potential. No evidence is observed for resonance-enhanced collisional cross sections, even at the low temperatures achieved, T < 1.0 K.     

Comparison of experimental time-of-flight spectra of the HF products from the F+H2 reaction with exact quantum mechanical calculations

High resolution HF product time-of-flight spectra measured for the reactive scattering of F atoms from n-H2(p-H2) molecules at collision energies between 69 and 81 meV are compared with exact coupled-channel quantum mechanical calculations based on the Stark-Werner ab initio ground state potential energy surface. Excellent agreement between the experimental and computed rotational distributions is found for the HF product vibrational states v'=1 and v'=2. For the v'=3 vibrational state the agreement, however, is less satisfactory, especially for the reaction with p-H2. The results for v'=1 and v'=2 confirm that the reaction dynamics for these product states is accurately described by the ground electronic state 1 (2)A' potential energy surface. The deviations for HF(v'=3, j' > or =2) are attributed to an enhancement of the reaction resulting from the 25% fraction of excited ((2)P(12)) fluorine atoms in the reactant beam.