The local potential energy (LPE) and local potential energy density (LPED) are Coulomb‐based QTAIM descriptors that assign interaction energies directly to individual bond critical points (BCPs), circumventing the locality limitation of global energy decomposition methods. Despite sharing the same algebraic expression, they differ by a single assumption—the zeroth‐order approximation—in which LPE implicitly sets the effective BCP volume to 1 Bohr
3
, collapsing LPED into an energy directly comparable to the supramolecular interaction energy (SME). Here, we provide the first rigorous derivation of this approximation, showing that its relative error is fully determined by |∇
2
ρ
bcp
|/
ρ
bcp
, yielding a mean of 13.38% ± 2.39% across 25 chemically diverse systems. Linear correlation analysis reveals LPED achieves
R
2
= 0.9607 with SME—marginally below
ρ
bcp
(
R
2
= 0.9701) yet substantially above VIR(bcp) (
R
2
= 0.8698), confirming that isolating the electron–nucleus attractive term enhances rather than degrades predictive performance. Quantitative benchmarking establishes clear, application‐dependent selection criteria for both descriptors.
Second-order Møller-Plesset theory (MP2) is the simplest wavefunction-based treatment of electron correlation and is a good compromise between accuracy and efficiency for evaluating the strength of many non-covalent intermolecular interactions. It has also been improved in accuracy and robustness by regularized methods...
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Core–valence (CV) correlation causes systematic milliangstrom-scale bond contractions in main-group molecules. We develop an analytic radial model for the structural all-electron–frozen-core (AE–FC) correction otherwise obtained from explicit second-order Møller–Plesset perturbation theory (MP2) calculations. Calibra...
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Solvation free energy (SFE) is a fundamental thermodynamic quantity governing biomolecular processes in solution. Although the atomic decomposition method derived from the Kirkwood charging formula enables site-resolved evaluation of SFE contributions, its application within the three-dimensional reference interaction...
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High-precision two-dimensional intermolecular potential energy surfaces (PESs) for Rg–CuF (Rg = Ar, Kr, Xe) were constructed at the coupled-cluster singles and doubles with non-iterative triples [CCSD(T)] level by employing aug-cc-pVXZ (X = D, T, Q) basis sets, and the energies were extrapolated to the complete basis s...
Accurate modeling of nonbonded interactions remains challenging because conventional force fields often provide inadequate descriptions of polarization and charge transfer. Here, we introduce a polarizable split-charge equilibration (PSQ) framework that combines localized charge flow with dipolar polarization, thereb...
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Complex matter, often partly soft and pliable, is the generic form of material systems. We must therefore generally call on density functional theory (DFT) to first predict the atomic structure before we can use it to also characterize (expected) properties. A recent range-separated hybrid (RSH) van Waals density funct...
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