Excited states of gaseous ions. IV. Potential energy surfaces of the H2O+ ion

Cross-sections of the potential energy hypersurfaces are reported for the four lower-lying states of the H₂O⁺ molecular ion. The symmetric dissociation of the ion has been investigated using the CNDO/2 method supplemented by a configuration interaction calculation. Self-consistent-field wave functions were calculated for the asymmetric dissociation using an extended basis of Gaussian-lobe functions. The values of the hydrogen exponents are found to be very sensitive to the molecular geometry. The calculated equilibrium H-O-H angle is 123° in the X?²B₁ state, nearly 180° in the X?A²A₁ state and 69° in the B?²B₂ state. The lower-lying quartet á ⁴B₁ is line entirely repulsive. The potential energy surface of the à ²A₁ state has a peculiar shape, characterized by two dissociation valleys.     

Infrared multiple photon dissociation of dichlorosilane: The production of electronically excited SiCl2

The infrared multiple photon excitation of SiH₂Cl₂, under collision-free and collisional conditions, via its v₂(a₁) SiH₂ bending fundamental resulted in dissociation and in an ultraviolet luminescence. The photodissociative products were found to be H₂ and SiCl₂ while the luminescence was shown to arise from a spontaneous one-photon radiative decay from electronically excited SiCl₂(¹B₁ → ¹A₁). The radiative lifetime of this transition has been measured as 4.5 μs and the collisional quenching rate of SiCl₂(¹B₁ → ¹A₁) by SiH₂Cl₂ as 2.6 × 10⁶ s^?1 Torr^?1. The reaction mechanism leading to product formation as well as models for populating the electronic state of the fragment are proposed and discussed in conjunction with present multiple photon dissociation theory.     

Photofragmentation of SnCl2 at 193 nm

Using photofragment spectroscopy the time of flight spectra and angular distributions for SnCl fragments, Sn and Cl atoms from the fragmentation of SnCl₂ have been measured at 193 nm. From the time, of flight it was found that dissociation takes place into SnCl (X ²Π) and Cl(²P) and that the SnCl fragment is highly vibrationally excited. To account for this effect we propose a mechanism, in which the upper potential surface has a saddle point at a greater Sn-Cl₂ distance than the ground state. The angular distribution exhibits an anisotropy parameter β = 0.21. A model was developed, based on a charge transfer from the p nonbonding orbitals on the Cl atoms to the p_x orbital on the Sn atom. The model predicts that A₁ → B₂ transitions dominate over A₁ → B₁ transitions and that A₁ → B₁ transitions are negligible in good agreement with the experimental observations.     

Configuration interaction study of the oscillator strenghts for the A1--- A1 and A1--- A1 transitions of the water molecule

Oscillator strengths for transitions between the ¹A₁ ground state of water and its ¹A₁ and ¹A₁ excited states are computed employing two different theoretical approaches. In one series of calculations a common orthonormal one-electron basis is employed for all of the above states, while in the other type of treatment two different, mutually non-orthogonal, sets are used; the multireference single- and double-excitation (MRD CI) method is employed in each case, with configuration selection, to generate the various electronic wavefunctions. It is found that the use of ground-state SCF MOs leads to poor convergence in the wavefunctions of the (Rydberg-type) ¹A₁ and ¹A₁ excited states and consequently also for the corresponding --- and --- f-values; this behavior is seen to be closely related to the near degeneracy of the two excited states, each of which is a mixture of the 3a₁ → 3sa₁ and 1b₁ → 3pb₁ configurations. Analogous computations with the ¹B₁¹b₁ → 3sa₁ MOs show much better convergence properties, and the resulting f-values compare well with what is obtained when state-specific orbital sets are employed separately for ground and excited states and non-orthonormal techniques are applied to compute the desired transition moments. These results tend to confirm previous findings which indicate conceptual and computational advantages for the calculation of excited-state wavefunctions and properties within the context of a state-specific theory. They also show that although the goal of eliminating the dependence of MRD CI calculations on the choice of MO basis is very nearly approached for energy quantities, it is less satisfactorily achieved for other properties, especially when the existence of nearly degenerate electronic states is a critical factor.     

A molecular orbital study of lithium ion association with bases. The excited carbonyl bases R2CO

SCF CI calculations have been performed to investigate Li^XXX association with excited bases R₂CO. Although association leads to large increases in n → π¹ transition energies, the complexes R₂COLi^XXX remain bound in the n → π¹ state, but are destabilized relative to the ground state. In the Li^XXX-urea complex, the n → π¹ A₂, state lies slightly above a charge-transfer π → σ^* A₂ state.     

Microwave—optical double resonance in the A1A2 excited state of thioformaldehyde

Microwave—optical double resonance experiments have been carried out on the 4_o¹ band of the $\text{A}$¹A₂$\text{X}$¹A₁ system of thioformaldehyde (H₂CS). More than 100 microwave and radiofrequency transitions have been observed in the $\text{A}$¹A₂ excited state. Many of these transitions are magnetically sensitive. Some of the excited state levels are perturbed by triplet levels and others by high vibrational levels of the ground state.     

1 Bu–2 Ag conical intersection in trans-butadiene: ultrafast dynamics and optical spectra

The potential-energy functions of the 1 ¹B_u and 2 ¹A_g excited valence states of trans-butadiene have been characterised by the CASPT2 method. Based on these ab initio data, a vibronic-coupling model describing the conical intersection of the 1 ¹B_u and 2 ¹A_g states has been constructed. UV resonance-Raman and absorption spectra have been calculated, employing the time-dependent approach. The time-dependent wave-packet calculations reproduce the expected ultrafast (≈30 fs) radiationless decay of the optically bright 1 ¹B_u state into the dark 2 ¹A_g state.     

Luminescence in near-thermal charge exchange. II. He+ + H2O and He+ + D2O

An ICR spectrometer fitted with synchronous photon counting equipment is used to study the emission produced by near-thermal (? 0.1 eV) collisions between He⁺ and H₂O (D₂). Within the investigated wavelength region, 185 to 500 nm, the only significant emission features are the A³Π (υ' ? 3) → X³Σ^? bands in OH⁺ and OD⁺, and the A²Σ⁺ → X²Π(0.0) band in OH and, possibly, in OD. The corresponding excitation rate constants represent only ? 2% of the total He⁺/H₂O (D₂O) charge transfer. The resonant electron-jump model for thermal-energy charge exchange is discussed in the light of recent information on the He⁺/H₂O reaction and on the excited states of H₂O⁺ and their excitation by electron and photon impact on H₂O (D₂O).     

Multiphoton ionisation spectroscopy of H2S: a reinvestigation of the 1B1-1A1 band at 139.1 nm

The 3 + 1 multiphoton ionisation (MPI) spectrum of the ¹B₁-¹A₁ transition in H₂S at 139.1 nm has been recorded in both linearly and circularly polarised light. The rotational structure shows marked differences from that of the one-photon absorption spectrum. Properties of the excited state revealed through analysis of this structure include confirmation of its ¹B₁ character, refined values for its A, B and C rotational constants and the operation of an energy-dependent predissociation mechanism. It is shown that the third-rank tensor component of the transition operator dominates over the first-rank component in this MPI band. The orbital nature of this ¹B₁ excited state is considered.     

The reactions of hydrogen atoms with bis(trifluoromethyl)disulfide

The reactions of hydrogen atoms produced by the mercury-photosensitized decomposition of H₂ with bis(trifluoromethyl)disulfide has been studied. The rate coefficient for the primary reaction, H + CF₃SSCF₃ → CF₃SH + CF₃S, was determined in competition with the reaction H + C₂H₄S → SH + C₂H₄ to have the value k = (3.0 ± 0.18) × 10¹⁴ exp[-(4560 ± 140)/RT] cm³ mol^?1 S^?1. The high A factor can be partially accounted for by assuming free rotation for the two CF₃ groups and the SCF₃ groups about the S—S bond in the transition state. The relatively high activation energy is attributed to inductive and orbital overlap effects. CH₃SH, H₂S, and CF₃SH all react with CF₃SSCF₃ to yield solid complexes which were not explored further.     

Photodeactivation paths in norbornadiene

The first high level ab initio quantum‐chemical calculations of potential energy surfaces (PESs) for low‐lying singlet excited states of norbornadiene in the gas phase are presented. The optimization of the stationary points (minima and conical intersections) and the recalculation of the energies were performed using the multireference configuration interaction with singles (MR‐CIS) and the multiconfigurational second‐order perturbation (CASPT2) methods, respectively. It was shown that the crossing between valence V₂ and Rydberg R₁ states close to the Franck–Condon (FC) point permits an easy population switch between these states. Also, a new deactivation path in which the doubly excited state with (π₃)² configuration (DE) has a prominent role in photodeactivation from the R₁ state due to the R₁/DE and the DE/V₁ conical intersections very close to the R₁ and DE minima, respectively, was proposed. Subsequent deactivation from the V₁ to the ground state goes through an Olivucci–Robb‐type conical intersection that adopts a rhombic distorted geometry. The deactivation path has negligible barriers, thereby making ultrafast radiationless decay to the ground state possible. © 2013 Wiley Periodicals, Inc.     

Photofragmentation of H2S in the first continuum

The dynamics of the photofragmentation of H₂S in the first continuum has been investigated at laser wavelengths 193, 222 and 248 nm. The HS fragments are produced mainly in υ = 0, as expected, but a non-negligible part of the HS radicals produced are vibrationally excited. The distribution of the vibrationally excited radicals peaks at υ = 3 or 4 at 193 nm and at υ = 2 at 222 nm. From the angular distribution of the H fragments it can be concluded that the anisotropy parameter β decreases with increasing wavelength. These results can be explained by a predissociation mechanism. Excitation in the first continuum takes place from the ¹A₁ ground state to the bound ¹B₁ state. This state is predissociated by a repulsive ¹A₂ state producing electronically ground-state H and HS fragments, of which the HS fragments can be vibrationally excited, resulting in a bimodal vibrational distribution. The increase of β with increasing wavelength is caused by a non-negligible lifetime in the ¹B₁ state.     

Theoretical investigation of the character of the electronic states of H2O along a linear dissociation path leading to OH + H

A series of MRD CI calculations is presented for the linear asymmetric dissociation of singlet states of the water molecule. The present calculations complement previous work on H₂O, providing further information on conical intersections in the higher excited states and on the nature and dissociation limits of the third ¹A' state in C_s symmetry, which is shown to correlate with the ion-pair limit (OH⁻ +H⁺). At large distances the ion-pair state is no longer the third ¹A' species as other states, corresponding to the OH(X ²Π) + H(2s,2p) dissociation limit, are then lower in energy.     

Structure and bonding of H3CCuH

The reaction CH₄ + Cu(²P) → H₃CCuH → H₃C-CU + H and H₃C + CuH has been subjected to ab initio SCF calculations within the RHF formalism using a split valence shell gaussian basis set. The three electronic states (²A₁m ²E and ²E) of H₃CCuH studied had C_3V symmetry. The molecular structure and computed properties of the H₃CCuH ground state (²A₁) suggested that this molecule can be considered as a methyl radical attached to a closed-shell CuH. The results also indicate that the formation of H₃CCuH may occur through either an insertion or via an abstraction mechanism, nevertheless, the insertion mechanism appears to be the most favoured.     

OH自由基的高精度量子化学研究

采用内收缩MRCI方法(Internally Contracted Multiconfiguration-Reference Configuration Interaction)研究了OH自由基, 计算得到其基态稳定构型的键长是0.09708 nm, 对应的实验值是0.096966 nm, 第一激发态的键长是0.10137 nm,实验值是0.10121 nm. 同时得到势能曲线PECs (Potential Energy Curve), 再分别由Murrell-Sorbie势能函数拟合计算和POLFIT程序计算得到OH自由基在基态X²Π和第一激发态A²Σ⁺时的光谱数据：平衡振动频率ω_e, 非谐性常数ω_eχ_e以及高阶修正ω_eY_e, 平衡转动常数B_e, 振转耦合系数α_e, 解离能D₀和垂直跃迁能量ν₀₀. 这些理论计算结果与最新的实验值非常吻合, 精确度比前人也有很大提高. 其中我们计算得到基态OH(X²Π)的解离能D₀＝35568.86 cm^－1, 第一激发态OH (A²Σ⁺)的解离能D₀＝18953.93 cm^－1, 从第一激发态A²Σ⁺ (ν＝0)到基态X²Π (v＝0)的垂直跃迁能ν₀₀＝32496.42 cm^－1.     

Collision-induced dissociation of dye-laser excited Li2(A 1Σ+u)

Li₂ molecules in a vapour cell were excited into the A ¹Σ⁺_u state using a dye laser set at 6103 Å. In the presence of a foreign gas Li(2 ²P) atoms were detected by means of the Li(3 ²D-2 ²P) transition which was simultaneously excited by the 6103 Å radiation. From the pressure dependence of the normalized Li fluorescence intensity absolute rate constants for collision-induced dissociation Li₂(A) → Li(2 ²P) by the five rare gases were determined. The results are compared with recent work on the analogous process in the Li₂(B ¹Π_u) state and with other systems.     

CH3S自由基H迁移异构化及脱H2反应的直接动力学研究

采用密度泛函方法(MPW1PW91)在6-311G(d,p)基组水平上研究了CH₃S自由基H迁移反应CH₃S→CH₂SH (R1), 脱H₂反应CH₃S→HCS＋H₂ (R2)以及脱H₂产物HCS异构化反应HCS→CSH (R3)的微观动力学机理. 在QCISD(t)/6- 311＋＋G(d,p)//MPW1PW91/6-311G(d,p)＋ZPE水平上进行了单点能校正. 利用经典过渡态理论(TST)与变分过渡态理论(CVT)分别计算了各反应在200～2000 K温度区间内的速率常数k^TST和k^CVT, 同时获得了经小曲率隧道效应模型(SCT)校正后的速率常数k^CVT/SCT. 结果表明, 反应 R1, R2 和R3的势垒△E^≠分别为160.69, 266.61和241.63 kJ/mol, R1为反应的主通道. 低温下CH₃S比CH₂SH稳定, 高温时CH₂SH比CH₃S更稳定. 另外, 速率常数计算结果显示, 量子力学隧道效应在低温段对速率常数的计算有显著影响, 而变分效应在计算温度段内对速率常数的影响可以忽略.     

Theoretical study of the π→π* excited states of linear polyenes: The energy gap between 11Bu+ and 21Ag− states and their character

Multireference perturbation theory with complete active space self-consistent field (CASSCF) reference functions is applied to the study of the valence π→π* excited states of 1,3-butadiene, 1,3,5-hexatriene, 1,3,5,7-octatetraene, and 1,3,5,7,9-decapentaene. Our focus was put on determining the nature of the two lowest-lying singlet excited states, 1¹B_u⁺ and 2¹A_g⁻, and their ordering. The 1¹B_u⁺ state is a singly excited state with an ionic nature originating from the HOMO→LUMO one-electron transition while the covalent 2¹A_g⁻ state is the doubly excited state which comes mainly from the (HOMO)²→(LUMO)² transition. The active-space and basis-set effects are taken into account to estimate the excitation energies of larger polyenes. For butadiene, the 1¹B_u⁺ state is calculated to be slightly lower by 0.1 eV than the doubly excited 2¹A_g⁻ state at the ground-state equilibrium geometry. For hexatriene, our calculations predict the two states to be virtually degenerate. Octatetraene is the first polyene for which we predict that the 2¹A_g⁻ state is the lowest excited singlet state at the ground-state geometry. The present theory also indicates that the 2¹A_g⁻ state lies clearly below the 1¹B_u⁺ state in decapentaene with the energy gap of 0.4 eV. The 0–0 transition and the emission energies are also calculated using the planar C_2h relaxed excited-state geometries. The covalent 2¹A_g⁻ state is much more sensitive to the geometry variation than is the ionic 1¹B_u⁺ state, which places the 2¹A_g⁻ state significantly below the 1¹B_u⁺ state at the relaxed geometry. © 1998 John Wiley & Sons, Inc. Int J Quant Chem 66 : 157–175, 1998     

Ab initio potential energy surfaces for BH+2

Preliminary ab initio calculations for the BH⁺₂ potential surface are presented. The reaction B⁺¹S) + H₂ → BH⁺ (B₂ (B²σ⁺) + H is shown to be most likely to occur for C_2v and near C_2v geometrics where there are avoided crossings between the 1 ¹A₁ and 2 ¹A₁ surfaces and between the 2 ¹A₁ and 3 ¹A₁ surfaces which should facilitate non-adiabatic transitions. Bent geometries are alos preferred for the reaction B⁺(¹S) + H₂ → BH⁺(A²π) + H for which there are avoided crossings in C₂ sysmmetry between surfaces correlating with 1 ¹A₁ and 1 ¹B₂ surfaces.