A rigorous energy partitioning scheme for analysis of molecular interactions

A rigorous method for partitioning the molecular interaction energy into classical electrostatic, charge-transfer, and wavefunction relaxation contributions is proposed. The energy components, defined with quantities central to density functional theory, are calculated with the help of the topological theory of atoms in molecules. Since the new scheme does not rely on Hilbert space partitioning, it is applicable to any level of electronic structure theory and it yields energy components that are true observables converging smoothly at the limit of a complete basis set. For this reason, the new method does not possess the deficiencies of the previously introduced Morokuma-Kitaura and Glendening-Streitwieser approaches. The results of several test calculations are compared with those obtained with the other energy partitioning schemes and found to exhibit superior numerical stability with respect to the quality of basis sets.

[1]  J. Cioslowski,et al.  The atomic softness matrix , 1994 .

[2]  Eric D. Glendening,et al.  Natural energy decomposition analysis: An energy partitioning procedure for molecular interactions with application to weak hydrogen bonding, strong ionic, and moderate donor–acceptor interactions , 1994 .

[3]  J. Cioslowski Electronic structure of the benzene–tetracyanoethylene complex: A synthesis of molecular orbital and density functional descriptions , 1994 .

[4]  J. Cioslowski,et al.  Electron flow and electronegativity equalization in the process of bond formation , 1993 .

[5]  J. Cioslowski,et al.  Electronegativities in situ, bond hardnesses, and charge-transfer components of bond energies from the topological theory of atoms in molecules , 1993 .

[6]  P. Surján,et al.  An observable-based interpretation of electronic wavefunctions: application to “hypervalent” molecules , 1992 .

[7]  I. Røeggen An analysis of hydrogen-bonded systems: (HF)2, (H2O)2 and H2O … HF , 1990 .

[8]  Steve Scheiner,et al.  Comparison of Morokuma and perturbation theory approaches to decomposition of interaction energy. (NH4)+…NH3 , 1990 .

[9]  R. Bader Atoms in molecules : a quantum theory , 1990 .

[10]  Ernest R. Davidson,et al.  Energy partitioning of the self‐consistent field interaction energy of ScCO , 1989 .

[11]  R. Parr Density-functional theory of atoms and molecules , 1989 .

[12]  L. Piela,et al.  Interpretation of the Hartree-Fock interaction energy between closed-shell systems , 1988 .

[13]  William H. Fink,et al.  Frozen fragment reduced variational space analysis of hydrogen bonding interactions. Application to the water dimer , 1987 .

[14]  Paul S. Bagus,et al.  A new analysis of charge transfer and polarization for ligand–metal bonding: Model studies of Al4CO and Al4NH3 , 1984 .

[15]  Friedrich Biegler-König,et al.  Calculation of the average properties of atoms in molecules. II , 1982 .

[16]  Paolo Arrighini Intermolecular Forces and Their Evaluation by Perturbation Theory , 1981 .

[17]  Keiji Morokuma,et al.  Why do molecules interact? The origin of electron donor-acceptor complexes, hydrogen bonding and proton affinity , 1977 .

[18]  K. Morokuma,et al.  The origin of hydrogen bonding. An energy decomposition study , 1977 .

[19]  K. Morokuma,et al.  Molecular orbital studies of electron donor-acceptor complexes. 3. Energy and charge decomposition analyses for several strong complexes: carbon monoxide-borane, ammonia-borane, methylamine-borane, trimethylamine-borane, and ammonia-boron trifluoride , 1976 .

[20]  Keiji Morokuma,et al.  Molecular Orbital Studies of Hydrogen Bonds. III. C=O···H–O Hydrogen Bond in H2CO···H2O and H2CO···2H2O , 1971 .

[21]  R. T. Sanderson,et al.  An Interpretation of Bond Lengths and a Classification of Bonds. , 1951, Science.