A comparison of time‐dependent and time‐independent quantum reactive scattering—Li+HF→LiF+H model calculations

Reactive scattering probabilities are computed over a wide range of collision energies for a model system based on the Li+HF→LiF+H reaction using both grid based time‐dependent and time‐independent quantum mechanical methods. The computations are carried out using a fixed Li–F–H angle which is chosen to be that at which the barrier to the chemical reaction is lowest. The calculated reaction probabilities for this system display many sharp features as a function of energy which are ascribed to scattering resonances. The time‐independent calculations have been carried out on a very dense energy grid, thus permitting detailed comparison between time‐independent and time‐dependent methods (in the latter case, a single computation of the wave packet dynamics provides information on the energy dependence over a given energy range). The results show that the time‐dependent calculations are capable of reproducing even the sharpest resonance features computed using the time‐independent method. The time‐dependent techniques are conceptually very simple and therefore easily implemented. The results presented also demonstrate that the grid based time‐dependent quantum mechanical methods used here are able to describe threshold energy dependence of reaction probabilities where the exit channel kinetic energy is effectively zero. The nature of some of the resonance structures are investigated by computing the time‐independent continuum wave functions at the ‘‘resonance’’ energies thus mapping out the nodal structure of the wave functions. The good agreement between time‐independent and time‐dependent methods is shown to be maintained when a centrifugal barrier is added to the potential to simulate the effect of nonzero orbital angular momentum.

[1]  R. Wyatt,et al.  Dynamics of the Collinear H+H2 Reaction. II. Energy Analysis , 1971 .

[2]  R. Kosloff,et al.  Absorbing boundaries for wave propagation problems , 1986 .

[3]  Antonio Laganà,et al.  A quasiclassical trajectory test for a potential energy surface of the Li+HF reaction , 1982 .

[4]  J. Kasper,et al.  Molecular Beam Reaction of K with HCl: Effect of Vibrational Excitation of HCl , 1971 .

[5]  G. G. Balint-Kurti,et al.  The approximate quantum mechanical calculation of reactive scattering cross sections: The fixed angle reactor model (FARM) , 1986 .

[6]  R. Dixon An efficient treatment of polar angles in three-dimensional wavepacket propagation with application to HCO→H+CO , 1992 .

[7]  H. Tal-Ezer,et al.  An accurate and efficient scheme for propagating the time dependent Schrödinger equation , 1984 .

[8]  Christopher H. Becker,et al.  Study of the reaction dynamics of Li+HF, HCl by the crossed molecular beams method , 1980 .

[9]  Gillian C. Lynch,et al.  Converged three‐dimensional quantum mechanical reaction probabilities for the F+H2 reaction on a potential energy surface with realistic entrance and exit channels and comparisons to results for three other surfaces , 1991 .

[10]  I. Noorbatcha,et al.  Vibrational threshold equal to the barrier height for an endothermic reaction: Li+FH→LiF+H on an ab initio potential‐energy surface , 1982 .

[11]  D. Neuhauser,et al.  Time dependent three‐dimensional body frame quantal wave packet treatment of the H+H2 exchange reaction on the Liu–Siegbahn–Truhlar–Horowitz (LSTH) surface , 1989 .

[12]  Antonio Laganà,et al.  Accurate 3D quantum reactive probabilities of Li+FH , 1993 .

[13]  A. Baram,et al.  Exact quantum mechanical three-dimensional reactive probabilities for the D + H2 system: variational calculations based on negative imaginary absorbing potentials , 1992 .

[14]  G. A. Parker,et al.  Quantum reactive scattering in three dimensions using hyperspherical (APH) coordinates. Theory , 1987 .

[15]  Antonio Laganà,et al.  Improved infinite order sudden cross sections for the Li+HF reaction , 1988 .

[16]  D. Neuhauser,et al.  Time-dependent (wavepacket) quantum approach to reactive scattering: Vibrationally resolved reaction probabilities for F+H2→HF+H , 1990 .

[17]  R. Kosloff,et al.  Dynamical atom/surface effects: Quantum mechanical scattering and desorption , 1984 .

[18]  D. F. Hays,et al.  Table of Integrals, Series, and Products , 1966 .

[19]  H. Loesch,et al.  Huge steric effect in the reaction Li+HF(v=1, j=1)→LiF+H , 1991 .

[20]  M. Baer,et al.  The time‐dependent Schrödinger equation: Application of absorbing boundary conditions , 1989 .

[21]  D. Kouri,et al.  Infinite order sudden approximation for reactive scattering. I. Basic l‐labeled formulation , 1979 .

[22]  M. Child ANALYSIS OF A COMPLEX ABSORBING BARRIER , 1991 .

[23]  William H. Press,et al.  Numerical recipes , 1990 .

[24]  A. Mulholland,et al.  The calculation of product quantum state distributions and partial cross sections in time dependent molecular collision and photodissociation theory , 1991 .

[25]  W. Miller,et al.  Quantum mechanical reaction probabilities via a discrete variable representation-absorbing boundary condition Green's function , 1992 .

[26]  U. Fano Effects of Configuration Interaction on Intensities and Phase Shifts , 1961 .

[27]  Yan Sun,et al.  Body frame close coupling wave packet approach to gas phase atom–rigid rotor inelastic collisions , 1989 .

[28]  S. Datz,et al.  Study of Chemical Reaction Mechanisms with Molecular Beams. The Reaction of K with HBr , 1955 .

[29]  A. Aguilar,et al.  Heavy-heavy-light limit and exchanged-atom isotopic effects in atom-diatom reactivity , 1992 .

[30]  R. Kosloff Time-dependent quantum-mechanical methods for molecular dynamics , 1988 .

[31]  Gabriel G. Balint-Kurti,et al.  The Fourier grid Hamiltonian method for bound state eigenvalues and eigenfunctions , 1989 .

[32]  C. Marston,et al.  Two computer programs for solving the Schrödinger equation for bound-state eigenvalues and eigenfunctions using the Fourier grid Hamiltonian method , 1991 .

[33]  R. Wyatt,et al.  Quantum dynamics of the H+D2→D+HD reaction: Comparison with experiment , 1991 .

[34]  M. Shapiro,et al.  Semiempirical potential surfaces for the alkali hydrogen‐halide reactions , 1979 .

[35]  Hiroki Nakamura,et al.  New implementation to approximate quantum mechanical treatment of atom-diatom chemical reactions , 1986 .

[36]  J. Polanyi,et al.  Effect of changing reagent energy on reaction dynamics. XI. Dependence of reaction rate on vibrational excitation in endothermic reactions HX(vreag)+Na→H+NaX(X≡F,Cl) , 1981 .

[37]  M. Shapiro,et al.  Theory of laser catalyzed reactions. I. Potential surfaces and transition dipoles in the Li+HCl reaction , 1986 .

[38]  G. A. Parker,et al.  Li+FH reactive cross sections from J=0 accurate quantum reactivity , 1993 .

[39]  R. Dixon,et al.  Photodissociation dynamics and emission spectroscopy of H2S in its first absorption band: A time dependent quantum mechanical study , 1990 .

[40]  G. Grossi Angular parametrizations in the hyperspherical description of elementary chemical reactions , 1984 .

[41]  G. G. Balint-Kurti,et al.  Potential energy surfaces for simple chemical reactions:. Application of valence-bond techniques to the Li + HF → LiF + H reaction , 1977 .

[42]  J. Bowman,et al.  Reduced dimensionality quantum calculations of mode specificity in OH+H2↔H2O+H , 1992 .

[43]  Antonio Laganà,et al.  Supercomputer algorithms for reactivity, dynamics and kinetics of small molecules , 1989 .

[44]  R. Wyatt,et al.  Quantum dynamics of the three‐dimensional Li+HF reaction: The bending corrected rotating nonlinear model , 1987 .

[45]  Antonio Laganà,et al.  Parallel calculations of approximate 3D quantum cross sections: the Li + HF reaction , 1991 .

[46]  The direct photodissociation of ClNO(S1): An exact three‐dimensional wave packet analysis , 1991 .

[47]  J. Connor,et al.  Differential cross sections for chemically reactive systems , 1970 .

[48]  G. G. Balint-Kurti,et al.  Parametrization of complex absorbing potentials for time-dependent quantum dynamics , 1992 .

[49]  S. Cuccaro,et al.  Hyper-spherical coordinate reactive scattering using variational surface functions , 1989 .

[50]  R. Dixon,et al.  Time-dependent quantum dynamics of reactive scattering and the calculation of product quantum state distributions — A study of the collinear F+H2(v=0) → HF(v′)+H reaction , 1991 .

[51]  Henry F. Schaefer,et al.  Potential energy surface for the Li+HF. -->. LiF+H reaction , 1980 .

[52]  Dong H. Zhang,et al.  A time‐dependent calculation for vibrational predissociation of H2HF , 1992 .

[53]  E. F. Hayes,et al.  Reactive differential cross sections in the rotating linear model. Reactions of fluorine atoms with hydrogen molecules and their isotopic variants , 1984 .

[54]  Robert B. Walker,et al.  An R matrix approach to the solution of coupled equations for atom–molecule reactive scattering , 1976 .

[55]  R. Dixon,et al.  Grid methods for solving the Schrödinger equation and time dependent quantum dynamics of molecular photofragmentation and reactive scattering processes , 1992 .

[56]  R. Dixon,et al.  Time-dependent quantum dynamics of molecular photofragmentation processes , 1990 .

[57]  Antonio Laganà,et al.  An accurate evaluation of the stationary points of the LiFH potential energy surface , 1989 .

[58]  Antonio Laganà,et al.  A bond-order LiFH potential energy surface for 3D quantum-mechanical calculations , 1988 .

[59]  Stephen K. Gray,et al.  Fragmentation mechanisms from three‐dimensional wave packet studies: Vibrational predissociation of NeCl2, HeCl2, NeICl, and HeICl , 1991 .

[60]  J. N. Murrell,et al.  Analytical potentials for triatomic molecules: VII. Application to repulsive surfaces , 1980 .

[61]  J. Rayez,et al.  Time-dependent calculation of the energy resolved state-to-state transition probabilities for three-atom exchange reactions , 1992 .

[62]  G. G. Balint-Kurti,et al.  Reflection and transmission of waves by a complex potential—a semiclassical Jeffreys–Wentzel–Kramers–Brillouin treatment , 1992 .

[63]  E. Garcia,et al.  A fit of the potential energy surface of the LiHF system , 1984 .

[64]  G. G. Balint-Kurti,et al.  Fixed angle reactor model calculations for the D+H2(v=0,1)→HD(v’=0,1,2)+H reaction , 1989 .

[65]  J. Hasted,et al.  Physics of Electronic and Atomic Collisions , 1963, Nature.