2008
DOI: 10.1002/9780470399545.ch1
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Computations of Noncovalent π Interactions

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Cited by 56 publications
(51 citation statements)
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“…24,25 and other journals. [26][27][28][29] Those references provide a convenient starting point for this review because the computationally demanding prescriptions for the reliable description of noncovalent interactions outlined therein also apply to the computational characterization of (H 2 O) n clusters. Many contemporary reviews of electronic structure methods for noncovalent interactions have emphasized the challenges associated with describing systems in which London dispersion forces play a dominant role, particularly interactions between aromatic molecules.…”
mentioning
confidence: 99%
“…24,25 and other journals. [26][27][28][29] Those references provide a convenient starting point for this review because the computationally demanding prescriptions for the reliable description of noncovalent interactions outlined therein also apply to the computational characterization of (H 2 O) n clusters. Many contemporary reviews of electronic structure methods for noncovalent interactions have emphasized the challenges associated with describing systems in which London dispersion forces play a dominant role, particularly interactions between aromatic molecules.…”
mentioning
confidence: 99%
“…Three-body contribution to interaction has been neglected so far but in order to check its influence on the results the interaction energy was calculated with an alternative scheme, which includes it. 38 The values are provided in the Supporting Information (Table S8). The data show that the three-body interaction adds only a mild contribution to the interaction energy.…”
Section: Interaction Energymentioning
confidence: 99%
“…91 The challenges to adapt efficient scaling wavefunction and DFT methods for treatment of dispersion have been the subject of several recent reviews in the literature. 84,[92][93][94][95][96] Among the empirical treatments developed are dispersion-corrected atom-centered potentials 97 and DFT-D. 80,[98][99][100] For common implementations of the former, a pseudo-potential optimized to replicate reference interaction energies is placed over each atom, thereby incorporating medium-range correlation but not capturing the correct asymptotic form, whereas for the latter, a damped atom-atom dispersion term is added to the total DFT energy, thereby accurately encoding the longrange attraction, yet necessitating a carefully tuned damping function to evenhandedly address double counting of the correlation energy across all system configurations and types of interaction. The exchange-hole dipole moment (XDM) is constructed similarly to DFT-D as a correction to the base electronic energy but, by modeling the instantaneous dipole that arises between an electron and its exchange hole, it generates dispersion coefficients that incorporate the effect of the chemical environment.…”
Section: Background On Simulation Approachesmentioning
confidence: 99%