Symmetric resonance charge transfer of Ar2+ IN Ar

Merging beams are used to measure cross sections for the reaction Ar²⁺ + Ar → Ar + Ar²⁺ at relative energies from 2 to 1000 eV. The results are in fair agreement with the theory of Fetisov and Firsov.     

Thermal energy charge transfer reactions of Ar+ ions with HBr and DBr molecules

HBr⁺ (A²Σ⁺-X²Π_i) and DBr⁺ (A²Σ⁺-X²Π_i) emissions are found up to v′=1 and v^′=2, respectively, from the thermal energy charge transfer reactions of Ar⁺ with HBr and DBr molecules in a flowing afterglow apparatus. Both A-state vibrational distributions have a peak at the lowest vibrational level, which are inconsistent with those expected from the energy resonance and/or Franck-Condon factors for ionization. This discrepancy is explained in terms of the distortion of target molecules by approach of reactant ions. Both A-state rotational distributions show that energies partitioned into rotation decrease with increasing vibrational levels, whereas the internal energy is nearly constant for all vibrational levels. The vibrational and rotational distributions obtained suggest that the reaction occurs at a relatively short distance and the product has a broad translational energy distribution.     

Low energy crossed beam study of the endothermic charge transfer reaction H+2(Ar,H2)Ar+

A crossed beam study of the title reaction if reported, from 0.45 to 7.8 eV. The reaction is predominantly translationally endothermic. At the lowest energy, there is evidence for two reaction paths: a long-range electron transfer and an intimate collision with electron transfer. Branching ratios for the competitive proton transfer reaction are presented.     

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).     

Crossed beam study of charge transfer of Ar+ with NO

The charge transfer reaction Ar⁺ (NO, Ar) NO⁺ was studied in a crossed beam experiment at collision energies above and below 1 eV (c.m.). Two mechanisms could be distinguished, an electron exchange process, and an intermediate complex formation; the latter involves moderate momentum exchange between the collision partners and is increasingly more important at low collision energies. Distributions of product translational energies showed that both mechanisms give rise to NO⁺ in the excited a ³Σ⁺ state in a quasi-resonant process. NO⁺ which originated via the complex mechanism was formed in Franck-Condon transitions in the a ³Σ⁺ state and, at higher collision energy, also in the b ³Π and w ³Δ states, in much less probable inelastic processes. These transitions are presumably obeyed because the NO bond distance is net perturbed during Ar⁺ approach.     

A State-selected study of the symmetric charge transfer reaction H2+ + H2

We have measured the relative total charge transfer cross sections of H₂⁺ + H₂ as a function of the vibrational state of H₂⁺, υ′_o = 0–4. using the crossed ion-neutral beam and high-resolution photoionization methods. The experimental results obtained at a center-of-mass collisional energy of 22.5 eV are found to be in excellent agreement with a recent theoretical study.     

Emission spectra produced from thermal energy charge transfer reactions of Ar+ ions with CS and PN radicals

CS⁺(B²Σ⁺-A²Π_i) and PN⁺(B²Σ⁺-X²Σ⁺) emissions were observed for υ′ = 0 and 1 from argon afterglow reactions of CS and PN radicals. The rotational constant (B₀) of the CS⁺(B) state was estimated to be 0.696±0.002 cm^?1 from the difference between band head and band origin. The dependence of each emission intensity on the voltage applied to the ion-collector grids and on the argon pressure indicated that Ar⁺ was a plausible candidate. Vibrational populations of the CS⁺(B) and PN⁺(B) states obtained from the emission spectra shifted to lower vibrational levels in comparison with those expected from the energy resonance and Franck-Condon factors for ionization. This is explainable as the distortion of target radicals by approach of reactant ions.     

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.     

An ab initio calculation of symmetric bending and stretching vibrational states of the H3O+ and D3O+ ions

Calculations are reported for the symmetric bending and stretching vibrational states of H₃O⁺ and D₃O⁺ including coupling between these two modes. The calculations were carried out by using a potential surface calculated by the SCF CI method and expressed in terms of symmetric internal coordinates. The transition energy of the ν₂ (1^? ← 0⁺) inversion mode is found to be 985 cm^?1, which is comparable to the experimental value of 954.417 cm^?1 observed by Haese and Oka. The calculated inversion doubling of the lowest state is 51 cm^?1.     

H2O? radicals trapped in Y-type zeolites

The results of CHDO/SP calculations do not support the detection of H₂O^– ions in MgY and CaY zeolites.

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CNDO/SP H₂O^– MgY CaY.

     

Photodissociation of O2+(H2O)

The photodissociation cross section of the weakly bound positive ion cluster O₂⁺(H₂O) has been measured at 15 discrete energies between 1.833 and 2.727 eV. Measurements indicate the cross section increases smoothly from 0.6 to 6 × 10^-18 cm² over this energy range. These cross section values are the largest reported for a positive ion cluster of atmospheric importance.     

The structure of H3O+TiF5−

Oxonium pentafluorotitanate was prepared by the reaction of H₂O with TiF₄ in HF. Single crystal x-ray diffraction studies on H₃O⁺TiF₅- show that the compound crystallizes in monoclinic form. The space group is C2/c and the unit cell dimensions are a = 14.528(5), b = 4.839(1), c = 13.798(5)A^o α = 115.59(5)^o with 8 formula units per unit cell.     

On the mechanism of the He+ + N2 thermal energy dissociative charge transfer reaction

ICR spectroscopy has been used to reinvestigate the He⁺ + N₂ charge transfer reaction at thermal energies. It is concluded that at least 60% of the N⁺ come from short lived excited (N₂⁺)^*.     

Effect of ionic charge on energy contributions to the interaction of an ion with a polar molecule: ab initio calculations for M⋯H2O (M = Mg,Mg+, Mg2+, Ca,Ca+, Ca2+)

For M?H₂O (M = Mg, Mg⁺, Mg²⁺, Ca, Ca⁺, Ca²⁺) various energy contributions (first-order, induction and charge-transfer, dispersion) are compared. Near the minimum, stability due to the first-order energy decreases and that due to dispersion increases from M²⁺ to M⁰. For M²⁺, dispersion represents only 1–7% of the total energy; it may reach 25% with M⁺ and is largely responsible for stability of the neutral complex.     

A crossed-beam study of low energy Ar + H2O collisions: Charge transfer and chemical reaction

Dynamics of Ar⁺ + H₂O collisions, charge transfer (H₂O⁺ formation) and chemical reaction (ArH⁺ formation), was investigated in crossed-beam experiments in the collision energy range 1–3 eV. The charge transfer occurs both by a simple-electron-jump mechanism and in impulsive intimate collisions. The distributions of relative translational energy of the products show that, most probably, the collisions are only slightly superelastic (by about 0.1 eV), and thus the product H₂O⁺ is highly internally excited. Formation of a small amount of H₂O⁺(B²B₂) in very inelastic collisions was observed. The chemical reaction is a direct process with characteristics of the spectator stripping mechanism.     

Detection of surface atoms by energy analysis of scattered primaries and recoiled secondaries from CsBr under Ar+ and Ar+ bombardment

Time-of-flight (TOF) and electrostatic sector analysis (ESA) have been used to measure particles scattered and sputtered by direct recoils and surface recoils during 3 keV Ar⁺ and 6 keV Ar²⁺ bombardment of CsBr at forward and backscattering angles. Charge fractions of scattered argon and recoiling surface atoms are obtained. Hydrogen and oxygen surface impurities are detected predominantly as directly recoiled neutrals.     

Kinetics and selectivity of the oxidation of alkanes in Cl2?H2O and Cl2?Hg2+?H2O solutions

Relative oxidation rate constants of several normal, iso-, cyclo-and methylcycloalkanes have been measured in Cl₂–H₂O and Cl₂–Hg²⁺–H₂O solutions at 343K. The selectivity of C–H bond dissociation in both systems is the same. HOCl is assumed to be the active species for the two systems.

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Cl₂–H₂O Cl₂–Hg²⁺–H₂O 343 , -,- ; C–H . , HOCl.

     

Vibrational energy transfer in H2 + He

A semiclassical approach is developed to study vibrational energy transfer in H₂ + He by use of the a priori interaction potential including all nonzero impact parameter collisions. The calculated values of the rate coefficient are found to be in excellent agreement with experimental data which are available in the temperature ranges 60–450 K and 1350-3000 K. The temperature dependence is shown to seriously deviate from the Landau-Teller prediction below 1000 K. The calculation was carried out over the temperature range of 30 to 10000 K.     

Structure and properties of H2CN,H2CC−, H2BO and H2CO+

Ab initio SCF—MO calculations are presented for H₂CN, H₂CC^?, H₂BO and H₂CO⁺, including geometry optimization. One-electron properties are presented and compared with experiment where possible, particularly ESR hyperfine data.