Evaluating common QTAIM and NCI interpretations of the electron density concentration through IQA interaction energies and 1D cross-sections of the electron and deformation density distributions
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Evaluating common QTAIM and NCI interpretations of the electron density concentration through IQA interaction energies and 1D cross-sections of the electron and deformation density distributions
Nine kinds of inter- and intramolecular interactions were investigated by exploring the topology of electron
density in the interatomic regions using standard protocols of QTAIM, IQA and NCI techniques as
well as in-house developed cross-sections of the electron and deformation density distributions. The first
four methods provide the properties of the resultant density distribution in a molecular system whereas
the later illustrates the process, inflow or outflow of density from fragments to the interatomic region of
an interaction on its formation in a molecular system. We used (i) the QTAIM-defined atomic interaction
line, AIL (presence or absence), (ii) IQA-defined interaction energy, EA;B
int , and its components, classical VA;B
cl
and exchange–correlation VA;B
XC term, (iii) NCI-defined isosurfaces to identify local regions of accumulated
(k2 < 0) or depleted (k2 > 0) density relative to immediate environment, and (iv) deformation density for
which Dq(r) > 0 indicates an inflow or otherwise an outflow of density on the interaction formation to
explore the nature of the interactions. We found (i) AILs for highly attractive and repulsive interactions,
regardless whether an inflow (Dq(r) > 0) or outflow of density into the interatomic region, (ii) no correlation
between the signs of k2 and EA;B
int ; both, highly repulsive and attractive, interactions might have
locally depleted density and vice versa, (iii) locally accumulated density (k2 < 0) does not imply that this
is the result of an inflow (Dq(r) > 0) of density and this equally applies to attractive and repulsive interactions
either with or without an AIL. Results obtained demonstrate that the molecular environment can
change the character of an interaction radically, from (i) attractive to repulsive, (ii) k2 < 0 to k2 > 0, or (iii)
Dq(r) > 0 to Dq(r) < 0; hence, none of the topological indices used here, either separately or combined,
can be used to definitely predict the (de)stabilizing nature of an interaction except highly repulsive ones
for which the absence of AIL, interatomic density depletion and outflow of density on interaction formation
are observed.