Global Method for Electron Correlation.

The current work presents a new single-reference method for capturing at the same time the static and dynamic electron correlation. The starting point is a determinant wave function formed with natural orbitals obtained from a new interacting-pair model. The latter leads to a natural orbital functional (NOF) capable of recovering the complete intrapair, but only the static interpair correlation. Using the solution of the NOF, two new energy functionals are defined for both dynamic (E^{dyn}) and static (E^{sta}) correlation. E^{dyn} is derived from a modified second-order Møller-Plesset perturbation theory (MP2), while E^{sta} is obtained from the static component of the new NOF. Double counting is avoided by introducing the amount of static and dynamic correlation in each orbital as a function of its occupation. As a result, the total energy is represented by the sum E[over ˜]_{HF}+E^{dyn}+E^{sta}, where E[over ˜]_{HF} is the Hartree-Fock energy obtained with natural orbitals. The new procedure called NOF-MP2 scales formally as O(M^{5}) (where M is the number of basis functions), and is applied successfully to the homolytic dissociation of a selected set of diatomic molecules, paradigmatic cases of near-degeneracy effects. The size consistency has been numerically demonstrated for singlets. The values obtained are in good agreement with the experimental data.

[1]  D. Mazziotti Approximate solution for electron correlation through the use of Schwinger probes , 1998 .

[2]  M. Piris A generalized self‐consistent‐field procedure in the improved BCS theory , 1999 .

[3]  T. Gilbert Hohenberg--Kohn theorem for nonlocal external potentials , 1975 .

[4]  K. Pernal The equivalence of the Piris Natural Orbital Functional 5 (PNOF5) and the antisymmetrized product of strongly orthogonal geminal theory , 2013 .

[5]  R. Donnelly On a fundamental difference between energy functionals based on first‐ and on second‐order density matrices , 1979 .

[6]  T. H. Dunning Gaussian basis sets for use in correlated molecular calculations. I. The atoms boron through neon and hydrogen , 1989 .

[7]  D. Mazziotti Structure of fermionic density matrices: complete N-representability conditions. , 2011, Physical review letters.

[8]  A. J. Coleman THE STRUCTURE OF FERMION DENSITY MATRICES , 1963 .

[9]  M. Piris,et al.  Perspective on natural orbital functional theory , 2014 .

[10]  X. López,et al.  A natural orbital functional for multiconfigurational states. , 2011, The Journal of chemical physics.

[11]  M. Piris A new approach for the two-electron cumulant in natural orbital functional theory , 2006 .

[12]  X. López,et al.  Communication: The role of the positivity N-representability conditions in natural orbital functional theory. , 2010, The Journal of chemical physics.

[13]  X. López,et al.  The intrapair electron correlation in natural orbital functional theory. , 2013, The Journal of chemical physics.

[14]  Mario Piris,et al.  Iterative diagonalization for orbital optimization in natural orbital functional theory , 2009, J. Comput. Chem..

[15]  Katarzyna Pernal,et al.  Reduced Density Matrix Functional Theory (RDMFT) and Linear Response Time-Dependent RDMFT (TD-RDMFT). , 2015, Topics in current chemistry.

[16]  M. W. Chase NIST-JANAF thermochemical tables , 1998 .

[17]  X. López,et al.  Spin conserving natural orbital functional theory. , 2009, The Journal of chemical physics.