A direct product decomposition approach for symmetry exploitation in many-body methods. I. Energy calculations

An analysis of the matrix contractions involved in many‐body perturbation theory and coupled‐cluster calculations leads to a convenient strategy for exploiting point group symmetry, by which the number of floating point operations can be reduced by as much as a factor of h2, where h is the order of the molecular point group. Contrary to a statement in the literature, the significant reduction in computation time realized in coupled‐cluster calculations which exploit symmetry is not due to nonlinearities in the equations. Rather, the savings of the fully vectorizable direct product decomposition (DPD) method outlined here is associated with individual (linear) contractions, and is therefore applicable to both linear and nonlinear coupled‐cluster models, as well as many body perturbation theory. In addition to the large reduction in floating point operations made possible by exploiting symmetry, core memory requirements are also reduced by a factor of ≊h2. Implementation of the method for both open and clos...

[1]  E. Fleischer X-Ray Structure Determination of Cubane , 1964 .

[2]  R. Pitzer Electron repulsion integrals and symmetry adapted charge distributions , 1973 .

[3]  P. C. Hariharan,et al.  The influence of polarization functions on molecular orbital hydrogenation energies , 1973 .

[4]  Isaiah Shavitt,et al.  Comparison of high-order many-body perturbation theory and configuration interaction for H2O , 1977 .

[5]  Michel Dupuis,et al.  Molecular symmetry and closed‐shell SCF calculations. I , 1977 .

[6]  P. Eaton,et al.  The Electronic Structure of Cubane (C8H8) as Revealed by Photoelectron Spectroscopy , 1978 .

[7]  Vibrational spectra of cubane and four of its deuterated derivatives , 1980 .

[8]  T. W. Cole,et al.  Vibrational spectra of cubane , 1981 .

[9]  Rodney J. Bartlett,et al.  The reduced linear equation method in coupled cluster theory. , 1981 .

[10]  R. Bartlett,et al.  A full coupled‐cluster singles and doubles model: The inclusion of disconnected triples , 1982 .

[11]  J. Almlöf,et al.  The molecular structure and spectra of cubane. An ab initio investigation , 1982 .

[12]  H. F. King,et al.  Molecular symmetry. IV. The coupled perturbed Hartree–Fock method , 1983 .

[13]  Peter Pulay,et al.  An efficient reformulation of the closed‐shell self‐consistent electron pair theory , 1984 .

[14]  J. M. Schulman,et al.  Ab initio heats of formation of medium-sized hydrocarbons. The heat of formation of dodecahedrane , 1984 .

[15]  Petr Čársky,et al.  Use of molecular symmetry in two‐electron integral transformation An MP2 program compatible with HONDO 5 , 1984 .

[16]  J. Watson,et al.  Tunable laser spectra of the infrared-active fundamentals of cubane , 1984 .

[17]  A. Almenningen,et al.  Cubane. molecular structure determined by gas-phase electron diffraction , 1985 .

[18]  Warren J. Hehre,et al.  AB INITIO Molecular Orbital Theory , 1986 .

[19]  S. Hermiller,et al.  Electronic structure of polyhedral alkanes , 1986 .

[20]  Rodney J. Bartlett,et al.  Fifth-Order Many-Body Perturbation Theory and Its Relationship to Various Coupled-Cluster Approaches* , 1986 .

[21]  Martin Head-Gordon,et al.  Quadratic configuration interaction. A general technique for determining electron correlation energies , 1987 .

[22]  Julia E. Rice,et al.  The closed‐shell coupled cluster single and double excitation (CCSD) model for the description of electron correlation. A comparison with configuration interaction (CISD) results , 1987 .

[23]  R. Bartlett,et al.  The full CCSDT model for molecular electronic structure , 1987 .

[24]  L. J. Schaad,et al.  Use of molecular symmetry in coupled‐cluster theory , 1987 .

[25]  J. Gauss,et al.  Implementation of analytical energy gradients at third- and fourth-order Møller-Plesset perturbation theory , 1987 .

[26]  R. Bartlett,et al.  Towards a full CCSDT model for electron correlation. CCSDT-n models , 1987 .

[27]  Julia E. Rice,et al.  An efficient closed-shell singles and doubles coupled-cluster method , 1988 .

[28]  G. Scuseria,et al.  A systematic theoretical study of harmonic vibrational frequencies: The single and double excitation coupled cluster (CCSD) method , 1988 .

[29]  Analytical MBPT(4) gradients , 1988 .

[30]  Curtis L. Janssen,et al.  An efficient reformulation of the closed‐shell coupled cluster single and double excitation (CCSD) equations , 1988 .

[31]  Rodney J. Bartlett,et al.  Analytic energy derivatives in many‐body methods. I. First derivatives , 1989 .

[32]  David H. Magers,et al.  Correlated studies of infrared intensities , 1989 .

[33]  R. Bartlett Coupled-cluster approach to molecular structure and spectra: a step toward predictive quantum chemistry , 1989 .

[34]  R. Walsh,et al.  Consequences of strain in (CH)8 hydrocarbons , 1989 .

[35]  R. Bartlett,et al.  The coupled‐cluster single, double, and triple excitation model for open‐shell single reference functions , 1990 .

[36]  R. Bartlett,et al.  Harmonic vibrational frequencies and infrared intensities from analytic fourth‐order many‐body perturbation theory gradients , 1991 .