Extension of the fourfold way for calculation of global diabatic potential energy surfaces of complex, multiarrangement, non-Born–Oppenheimer systems: Application to HNCO(S0,S1)

The fourfold way is a general algorithm for generating diabatic electronic wave functions that span the same space as a small set of variationally optimized adiabatic electronic wave functions and for using the resulting diabatic wave functions to generate diabatic potential energy surfaces and their couplings. In this paper we extend the fourfold way so it is applicable to more complex polyatomic systems and in particular to the calculation of global potential energy surfaces for such systems. The extension involves partitioning the active space into three blocks, introducing restricted orbital rotation within two of the blocks, introducing a specific resolution of the subspace containing molecular orbitals that are doubly occupied in all dominant configuration state functions, and introducing specific orientations of the coordinate systems for reference molecular orbitals and resolution molecular orbitals. The major strength of the improved method presented in this paper is that it allows the diabatic molecular orbitals to exhibit a gradual change of chemical character with smooth deformation along the reaction coordinate for a change of chemical arrangement while preserving the orbital character required for a physical ordering of the orbitals. This feature is required for the convenient construction of global potential energy surfaces for non-Born–Oppenheimer rearrangements. The resulting extended algorithm is illustrated by calculating diabatic potential energy surfaces and couplings for the two lowest singlet potential energy surfaces of HNCO.

[1]  D. Truhlar,et al.  Direct diabatization of electronic states by the fourfold way. II. Dynamical correlation and rearrangement processes , 2002 .

[2]  Donald G. Truhlar,et al.  Properties of nonadiabatic couplings and the generalized Born–Oppenheimer approximation , 2002 .

[3]  D. Truhlar,et al.  The direct calculation of diabatic states based on configurational uniformity , 2001 .

[4]  D. Yarkony Intersecting conical intersection seams in tetra-atomic molecules: the S1–S0 internal conversion in HNCO , 2001 .

[5]  D. Yarkony Characterizing the local topography of conical intersections using orthogonality constrained parameters: Application to the internal conversion S1→S0 in HNCO , 2001 .

[6]  Thomas Müller,et al.  High-level multireference methods in the quantum-chemistry program system COLUMBUS: Analytic MR-CISD and MR-AQCC gradients and MR-AQCC-LRT for excited states, GUGA spin–orbit CI and parallel CI density , 2001 .

[7]  Martina Bittererová,et al.  On the S1→S0 internal conversion in the photodissociation of HNCO: the role of the NC stretch as a promoting mode , 2000 .

[8]  Martina Bittererová,et al.  On the internal conversion in the photodissociation of HNCO , 1999 .

[9]  O. Prezhdo Mean field approximation for the stochastic Schrödinger equation , 1999 .

[10]  R. Schinke,et al.  The photodissociation of HNCO in the S1 band: A five-dimensional classical trajectory study , 1999 .

[11]  K. Morokuma,et al.  Ab initio theoretical studies on photodissociation of HNCO upon S1(1A″)←S0(1A′) excitation: The role of internal conversion and intersystem crossing , 1999 .

[12]  K. Drukker,et al.  Quantum scattering study of electronic Coriolis and nonadiabatic coupling effects in O(1D)+H2→OH+H , 1999 .

[13]  Luis Serrano-Andrés,et al.  The multi-state CASPT2 method , 1998 .

[14]  K. Ruedenberg,et al.  Determination of diabatic states through enforcement of configurational uniformity , 1997 .

[15]  P. Halvick,et al.  Ab initio quasidiabatic states for the reaction N + CH → NC + H , 1997 .

[16]  M. Persico,et al.  Ab initio determination of quasi-diabatic states for multiple reaction pathways , 1997 .

[17]  David E. Keyes,et al.  Domain-Based Parallelism and Problem Decomposition Methods in Computational Science and Engineering , 1995 .

[18]  Ernest R. Davidson,et al.  Considerations in constructing a multireference second‐order perturbation theory , 1994 .

[19]  Haruyuki Nakano,et al.  Quasidegenerate perturbation theory with multiconfigurational self‐consistent‐field reference functions , 1993 .

[20]  K. Ruedenberg,et al.  A quantum chemical determination of diabatic states , 1993 .

[21]  I. Petsalakis,et al.  Diabatic potentials for the 1 1A″ and 2 1A″ states of H2S , 1993 .

[22]  Robert B. Murphy,et al.  Generalized Mo/ller–Plesset and Epstein–Nesbet perturbation theory applied to multiply bonded molecules , 1992 .

[23]  Kimihiko Hirao,et al.  Multireference Møller—Plesset perturbation theory for high-spin open-shell systems , 1992 .

[24]  Kimihiko Hirao,et al.  Multireference Møller-Plesset method , 1992 .

[25]  Björn O. Roos,et al.  Second-order perturbation theory with a complete active space self-consistent field reference function , 1992 .

[26]  L. Cederbaum,et al.  Quasidiabatic states from ab initio calculations by block diagonalization of the electronic Hamiltonian: Use of frozen orbitals , 1991 .

[27]  R. Buenker,et al.  Ab initiostudy of NO2: Part II: Non-adiabatic coupling between the two lowest2A′ states and the construction of a diabatic representation , 1990 .

[28]  F. Gadéa,et al.  Approximately diabatic states: A relation between effective Hamiltonian techniques and explicit cancellation of the derivative coupling , 1990 .

[29]  Peter Pulay,et al.  Generalized Mo/ller–Plesset perturbation theory: Second order results for two‐configuration, open‐shell excited singlet, and doublet wave functions , 1989 .

[30]  C. Mead,et al.  On the form of the adiabatic and diabatic representation and the validity of the adiabatic approximation for X3 Jahn–Teller systems , 1985 .

[31]  J. Malrieu,et al.  The use of effective Hamiltonians for the treatment of avoided crossings. II. Nearly diabatic potential curves , 1984 .

[32]  B. Schneider,et al.  Multireference many‐body perturbation theory: Application to O2 potential energy surfaces , 1983 .

[33]  P. Löwdin,et al.  New Horizons of Quantum Chemistry , 1983 .

[34]  C. Mead,et al.  Conditions for the definition of a strictly diabatic electronic basis for molecular systems , 1982 .

[35]  B. Roos,et al.  A simple method for the evaluation of the second-order-perturbation energy from external double-excitations with a CASSCF reference wavefunction , 1982 .

[36]  B. Roos,et al.  A complete active space SCF method (CASSCF) using a density matrix formulated super-CI approach , 1980 .

[37]  Richard B. Bernstein,et al.  Atom - Molecule Collision Theory , 1979 .

[38]  H. Schaefer Methods of Electronic Structure Theory , 1977 .

[39]  R. Berry,et al.  Theory of Elementary Atomic and Molecular Processes in Gases , 1975 .

[40]  T. H. Dunning Gaussian Basis Functions for Use in Molecular Calculations. III. Contraction of (10s6p) Atomic Basis Sets for the First‐Row Atoms , 1970 .

[41]  F. Smith,et al.  DIABATIC AND ADIABATIC REPRESENTATIONS FOR ATOMIC COLLISION PROBLEMS. , 1969 .

[42]  W. Lichten Resonant Charge Exchange in Atomic Collisions , 1963 .