Abstract
The topological behaviour of the electron density (ρ) derived from correlated wavefunctions is analyzed for Li2, Li4(D 2h ), Li5(C2v ), and Li6(D 3h ) planar clusters considered in their optimal geometry. The topology ofρ of Li2 shows an unusual maximum located at the midpoint of the Li-Li equilibrium distance. The occurrence of maxima ofρ at positions other than nuclei (characteristic also for planar Li4, Li5, and Li6 clusters) implies the existence of molecular subspaces (bounded by zero-flux surfaces in the gradient ofρ at each point of the surface) which do not enclose a nucleus but still satisfy the virial theorem. This result provides a generalization of Bader's quantum theory of atoms in molecules to systems in which electrons behave partially as mobile metallic electrons. Maxima ofρ preferentially occur within the triangles (two in Li4, two in Li5 and three in Li6), while the number of maxima at the Li-Li midpoint is minimized: they are present only when the existence of a maximum within a triangle is not allowed because of the non suitable formal valence of the Li atoms involved. All the cluster atoms are bonded to “attractors” associated with the unusualρ maxima, but they are not directly bonded to each other. The cluster stability is found to be dependent on the number and kind ofρ maxima. The topological analysis clearly differentiates between Li atoms which occupy different coordination positions within the cluster in terms of their local and average properties. In particular, the degree ofsp hybridization is markedly different for Li atoms with two, three or four nearest neighbors. This implies that a unique definition of a reference valence state for atoms in clusters is impossible. As a consequence, the use of standard electron density difference maps for the description of the charge accumulation and depletion process which ensues the chemical bonding, appears rather questionable.
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An AIMPAC modified version for GOULD-SEL computers was actually used (Gatti C unpublished work)
A basin is defined as the region enclosed by all the gradient paths (traced out by following the gradient vector ofρ from some intial point) which terminate at the attractor (see Appendix)
It is interesting to note that also the ground stateX 1Σ +g of C2 exhibits a maximum at the C-C midpoint, at variance with the corresponding bonds in saturated and unsaturated hydrocarbons, which all show the usual (3, −1) bond critical point (an exceptional maximum in C2H2 X 1Σ +g disappears after the inclusion of electron correlation at the SD CI 6-31G** level [27a]). However, theρ M/ρS value (see text) is exceedingly small (1.008) (MRD CI optimal geometry, including HF canonical valence and virtual orbitals in the active space and employing [9s5p1d/4s2p1d] [27b] basis set) and the maximum could be perhaps removed considering a wavefunction of even higher quality
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Actually the two maxima do not normally coincide in location (see Appendix); for example, by lengthening the Li-Li bond to 6 au, a (3, −1) point in −∇2 ρ is created at theρ maximum located at the Li-Li midpoint, while the −∇2 ρ bonded maximum remains nearly fixed at a distance of 2.55 au from Li (Table 4)
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The charge density values at the non-nuclear maximum and at its closest saddle point (labelled as 3 in Fig. 4a) are very similar for BasisB (1.13 and 1.12 au, respectively). This fact could suggest that a singularity inρ is forming and that a structure change is at hand [18b, 31]. However, this is not the case as the softest in-plane curvatures of the charge density at the two critical points are associated with principal axes which are orthogonal to the line joining the two critical points
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The substantial in-plane bond ellipticity of cyclopropane, which resembles in some respect the case of the central region of Li4, provides a physical basis for its peculiarπ functionality [26]
Moments other than the monopole (the net charge) may be determined for an atom in a molecule by averaging the corresponding operator over the charge density on the subspace. Here we are interested with the diagonal components of the traceless quadrupole moment tensor, defined as\(Q_{ii} (\Omega ) = - e\int {_\Omega \rho (3i^2 - r^2 )d\tau ,} i = x,y,z.\) For a spherical distribution, theQ ii are identically equal to zero, while a negativeQ ii value agrees with an accumulation of charge in theii direction at the expense of the direction(s) associated with a positiveQ ii component
The bond paths which connect Li(4nn) to the non-nuclear attractors 2 and the non-nuclear attractors among themselves, form a four-membered ring, enclosing a surface within which the charge density attains a minimum value at the (3, +1) critical point (labelled as 8 in Fig. 5a). The principal axis associated with theλ 1 curvature of the ring critical point gives the direction of the line shared by the boundary surfaces of the three non-nuclear and Li(4nn). Two other three-membered rings are recognizeable in Fig. 5a, having as vertices a Li(3nn), a non-nuclear attractor like 2 and the non-nuclear attractor 1 which is in common to the two rings
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Dedicated to Professor J. Koutecký on the occasion of his 65th birthday
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Gatti, C., Fantucci, P. & Pacchioni, G. Charge density topological study of bonding in lithium clusters. Theoret. Chim. Acta 72, 433–458 (1987). https://doi.org/10.1007/BF01192234
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DOI: https://doi.org/10.1007/BF01192234