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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 3551-3558 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Classical molecular dynamics simulations of F2 photodissociation in a host Ar crystal are presented. At temperature T=12 K, the photodissociation yield shows a sharp threshold for an excess energy of ∼0.6 eV, and it reaches nearly unity for excess energies above 2 eV. For a given excess energy, the quantum yield at 4 K is higher than a 12 K, and is predicted to remain finite even at 0 K. The transition state for photofragment exit from the reagent cage is found to be located in well-defined windows in the unit cell of the surrounding solid. The quantum yields (or photodissociation probabilities) are extremely high, especially at low T, in comparison with the values found in previous studies, e.g., for Cl2 in Xe and in Ar. Indeed, for high excess energy the near-unit quantum yields indicate the virtual absence of an inhibiting cage effect on the reaction. The anomalous behavior of F2 in Ar is attributed to the short effective range of the repulsive F/Ar interaction, which enables the F atom to exit the cage and migrate in the crystal. It is also due in part to the F/Ar attractive potential, which is found strong enough to focus and stabilize the migration of the F product in "channels'' within the lattice, following photolysis. Classical trajectories show long-range migration of the product atoms, of the scale of 30 A(ring), following the initial impulse provided by the photodissociation. This is the first system for which such long-range impulse-induced migration was found. The results of the simulations are analyzed focusing on the role of the initial state of F2 in the crystal, on the final sites occupied by the product atoms, and on the migration dynamics. Implications of the results for mechanisms of reactions in solids are discussed.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 6728-6736 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Vibrational energies and eigenfunctions of Ar3, including some pertaining to highly excited states, are computed, and insights into their dynamical and structural properties are obtained. The method used employs the vibrational self-consistent-field (SCF) theory in hyperspherical coordinates as a first approximation. Exact results are obtained by configuration interaction, using the SCF states as an efficient basis. A focal point of the study is the effect of three-body potentials on the vibrational spectrum. Axilrod–Teller and other three-body potentials are used to examine this. It is found that the effect of three-body forces on the spectrum is substantial, and larger than effects due to uncertainties in the presently known two-body Ar–Ar potentials. This suggests that experimental spectroscopy of Ar3 may be used to determine reliable three-body forces among Ar atoms. It is also shown that the three-body double-dipole–quadrupole interaction, while less important than the Axilrod–Teller one, has a significant effect on the vibrational spectrum. Finally, a detailed analysis is made of the Ar–Ar distance distributions in the various states, of the structural distributions of Ar3, and of the properties of the wave functions. We find that the wave functions show well-ordered nodal patterns even for the highly excited large-amplitude states. Thus, these states do not correspond qualitatively to "liquid-like'' behavior of the cluster.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 6484-6490 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The photodissociation dynamics of a collinear model of the van der Waals cluster Xe–HI is used as a testing ground for time-dependent self-consistent field (TDSCF) approximations. In this study, the quantum-mechanical TDSCF and a combined classical/quantal TDSCF (in which the light atom is treated quantum mechanically, the heavy atoms are treated classically) are compared to numerically exact wave packet calculations. Very good agreement is found between the TDSCF approximations and the exact result over the entire subpicosecond time duration of the process. In particular, all the properties related to the quantal degree of freedom in the combined quantal/classical TDSCF method reproduce almost perfectly the exact results. However, the classical mode in the hybrid approximation is somewhat less well described due to insufficient representation of energy transfer between the modes. The conclusions are very promising as to the applicability of TDSCF methods, in particular the hybrid quantal/classical scheme to more complex systems in which only a few degrees of freedom can be treated quantum mechanically.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 887-893 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Molecular-dynamics (MD) simulations are used to study the vibrational properties of ICl adsorbed on an MgO(001) surface, and the photodissociation dynamics of the molecule after excitation to a 1Π electronic state. The electronic ground-state simulations show that ICl lies nearly parallel to the surface and occupies a single orientational site at surface temperatures below 150 K. Above 350 K the molecule hops between two orientational sites on the surface, and at 500 K full rotational diffusion of the adsorbate in the surface plane occurs. The multiplicity of sites and the onset of rotational diffusion at high T were found to greatly affect the dissociation dynamics and its temperature dependence. The photodissociation simulations show that only a fraction of the Cl atoms and some of the I atoms (which have a much higher binding energy) leave the surface following photolysis (at these energies). The fraction of Cl atoms leaving the surface subsequent to photodissociation at 50 K is ∼0.5, and it decreases as T is raised to 150 K. The trajectories show that Cl atoms leave the surface preferentially for initial ICl orientations in which the Cl end "points down.'' This orientation ensures that the escaping atom rapidly collides with the surface atoms. Momentum transfer due to surface local roughness is crucial for the Cl to acquire "escape velocity'' normal to the surface. The angular intensity distribution of the Cl atoms is sensitive to surface corrugation, and the energy distribution of the photofragments strongly reflects the Cl/surface collision stage of the process. It is concluded that photodissociation experiments can provide information both on surface local structure and on photofragment/surface interaction and energy transfer.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 7708-7715 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The photodissociation of an isolated IBr molecule adsorbed on an MgO(001) surface is studied theoretically. The calculations correspond to an excitation into the repulsive (Y0+) /quasibound (B 3Π0+) electronic state manifold, which may lead to the production of excited state or ground state bromine atoms. Using a quantum scattering method, we calculate the photoabsorption line shape for this process and the [Br]/[Br*] branching ratio as a function of photoexcitation wavelength. In the quantum calculations the IBr stretching was treated exactly, the in-plane librational mode was treated in the sudden approximation, and all other adsorbate and crystal modes were frozen. In addition, we studied the photodissociation process classically in order to explore the validity of freezing most of the modes. In the quantum calculations it was found that the width and intensities of the structured part of the absorption profile were greatly increased compared with the gas-phase photodissociation process. This was attributed to the stabilization of both electronic states by the molecule/surface interactions. The classical results showed that at least semiquantitatively, the crystal modes are unlikely to affect the process on the timescale pertinent to the calculated line shape.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 4242-4252 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Photodissociation of ICN by UV excitation in solid and liquid Ar is studied by molecular dynamics simulations. The focus is on the differences between the cage effects on the CN photoproduct in the two phases, and on the excited state isomerization ICN*→INC* dynamics in the solid matrix. Nonadiabatic transitions are neglected in this first study. The main results are: (1) No cage exit of the CN product is found in solid Ar, even in simulations at temperatures close to melting and for large excess energies. The result is in accord with recent experiments by Fraenkel and Haas. This should be contrasted with the large cage-exit probabilities found in many systems for atomic photofragments. The result is interpreted in terms of geometric and energy transfer considerations. It is predicted that complete caging of diatomic and larger photofragments will be typically the case for photodissociation in rare-gas matrices. (2) Almost 100% cage-exit probability for the CN product is found for ICN photolysis on the 1Π1 potential surface in liquid Ar. On the other hand, photolysis on 3Π0+ potential surface does not lead to cage exit on a time scale of 15 ps. The large differences between the reaction in the solid and in the liquid, and between the behavior of the process on the 3Π0+ and the 1Π1 potentials, respectively in the liquid, are interpreted. (3) CN rotational dynamics and subsequent relaxation leads to isomerization in the excited electronic states. On the 3Π0+ potential surface one finds after t(approximately-greater-than)0.5 ps roughly equal amounts of the ICN and INC isomers. On the 1Π1 surfaces only INC is found after t(approximately-greater-than)3.5 ps. This is explained in terms of the barriers for CN rotation in the two excited states, and in terms of the time scales for rotational relaxation. The results throw light on the differences between cage effects for photochemical reactions in solid and in liquid solution, and on cage-induced isomerization dynamics in solid matrices.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 1975-1987 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A general method for studying transition state spectroscopy and dynamics in hydrogen atom transfer reactions is presented. This approach is based on the time-dependent self-consistent field (TDSCF) approximation and is applied to a study of the ClHCl− photodetachment experiments of Metz et al. [Metz et al., J. Chem. Phys. 88, 1463 (1988)]. Comparison of results of exact time-dependent and TDSCF calculations are made for collinear and three-dimensional (J=0) approximations for the quantum dynamics. When ClHCl is constrained to be collinear, the TDSCF calculation overcorrelates the motions in the H atom displacement and ClCl extension coordinates. This results in relatively poor agreement with the exact result for many properties of the wave function. In contrast, when the system is propagated in the three vibrational coordinates of the system, the transition state dynamics are effectively over much more rapidly. Consequently, the TDSCF approximation yields results of very good quantitative accuracy over the time required for most of the wave function to decay off of the transition state. Comparison is also made between the wave function that results from the exact propagation and from TDSCF when the wave function in the ClCl stretch coordinate is approximated by a Gaussian wave packet. Here the magnitude of the overlap between the two TDSCF wave functions in the H atom coordinates, for quantum and semiclassical propagations of the wave function in the ClCl distance coordinate, is greater than 0.98 over the time of the propagations. These TDSCF calculations are repeated for a wave function that is approximated by a product of a two-dimensional wave function in the hydrogen atom coordinates and a one-dimensional wave function in the ClCl extension coordinate and even better quantitative agreement with the exact propagation is achieved. The success of this method for studying ClHCl gives us confidence that TDSCF will provide a general powerful tool for studies of hydrogen and proton transfer reactions in large systems.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 343-355 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The role of solvent effects in association reactions is studied in atom-cluster collisions. Classical trajectory studies of the systems H+Cl(Ar)n (n=1,12) are used to investigate the influence of size, structure, and internal energy of the "microsolvation'' on the H+Cl association reaction. The following effects of solvating the chlorine in an Arn cluster are found. (1) In the H+ClAr system there is a large "third body'' effect. The single solvent atom stabilizes the newly formed HCl molecule by removing some of its excess energy. The cross section found at low energies is a substantial fraction of the gas-kinetic cross section. The molecule is produced in highly excited vibrational-rotational states. (2) Some production of long-lived HCl...Ar complexes, with lifetimes of 1 ps and larger, is found for the H+ClAr collisions. Weak coupling stemming from the geometry of the cluster is the cause for long life times. These resonance states decay into HCl+Ar. (3) At low collision energy (E=10 kJ/mol) for H+Cl(Ar)12, the H+Cl association shows a sharp threshold effect with cluster temperature. For temperatures T≥45 K the cluster is liquidlike, and the reaction probability is high. For T≤40 K the cluster is solidlike, and there is no reactivity. This suggests the potential use of reactions as a signature for the meltinglike transition in clusters. (4) At high collision energies (E=100 kJ/mol) H atoms can penetrate also the solidlike Cl(Ar)12 cluster. At this energy, the solid–liquid phase change is found not to increase the reaction probability.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 8408-8417 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Molecular dynamics (MD) computer simulations are carried out for scattering of high-energy Xe atoms off liquid squalane, and the results are compared with those of molecular-beam scattering experiments. A crude model for squalane is adopted, describing the hydrocarbon chain molecule as a sphere, and ignoring the role of internal modes. Good overall agreement is found between the results of the simulations and experiment, both for angular distributions and for trends in energy transfer properties. In particular, excellent agreement is obtained for the dependence of the energy transfer on the deflection angle for in-plane scattering. Theory predicts less trapping events than found experimentally, probably due to the crude model adopted for the squalane molecules. The partial success of the model in predicting some properties and not others is discussed. The other main conclusions of the study are (1) The instantaneous local structure of the liquid surface is highly corrugated, giving rise to a broad angular distribution and to extensive out-of-plane scattering. (2) High-energy atoms undergo both a trapping desorption and also direct inelastic scattering, the latter yielding information on liquid structure. (3) The angular distribution of atoms at a selected final velocity is sensitive to the local structure and dynamics of the surface. (4) The direct scattering can be conveniently interpreted in terms of contributions from single, double, and multiple collision events, these being roughly equal in relative weight. Forward scattering at grazing angle is dominated by single collisions, while double and multiple collisions have higher contribution at other directions. The double collision contribution in particular contains structural information. (5) There is a substantial yield per collision for sputtering of the squalane-like soft spheres. These results provide insight into the dynamics of gas–liquid collisions, and indicate the usefulness of beam scattering as a tool for studying liquid structure and dynamics.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 2577-2591 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The structure and stability of clusters of a boron atom with one to eight H2 molecules is investigated. For the simplest BH2 clusters, the lowest ab initio adiabatic potentials for o-H2 and p-H2 interacting with a boron atom are used. For the larger clusters (n=2–8), the p-H2 is treated as a sphere, and the total potential is taken to be the sum of pairwise additive B–H2 and H2–H2 interactions which include, in the former case, an anisotropy due to the orientation of the unpaired B 2p electron. This electronic interaction is considerably more attractive when H2 approaches the B atom in a plane perpendicular to the orientation of the 2p orbital. The local and global minima on these potential surfaces were located and diffusion quantum Monte Carlo simulations were used to determine the energies and properties of the ground state wave functions for these B–(H2)n clusters. For the B(H2) cluster, a comparison is made with the results of variational calculations.
    Type of Medium: Electronic Resource
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