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Charge density topological study of bonding in lithium clusters

Part I: Planar Li n clusters (n=4, 5, 6)

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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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References and notes

  1. Koutecký J & Fantucci P (1986) Chem Rev 86:539

    Google Scholar 

  2. Morse MD (1986) Chem Rev 86:1049

    Google Scholar 

  3. Fantucci P, Balzarini P (1978) J Mol Catal 4:337

    Google Scholar 

  4. Beckmann HO, Koutecký J, Botscwhina P, Meyer W (1979) Chem Phys Lett 67:119

    Google Scholar 

  5. Beckmann HO, Koutecký J, Bonacic-Koutecký V (1980) J Chem Phys 73:5182

    Google Scholar 

  6. Flad J, Stoll H, Preuss H (1979) J Chem Phys 71:3042

    Google Scholar 

  7. Martins JL, Buttet J, Car R (1984) Phys Rev 53:655; Martins JL, Buttet J (1985) Phys Rev B 31:1804

    Google Scholar 

  8. Rao KB, Jena P (1985) Phys Rev B 32:2058

    Google Scholar 

  9. Ray AK, Fry JL, Myles CW (1985) J Phys B 18:381

    Google Scholar 

  10. Boustani I, Pewestorf W, Fantucci P, Koutecký J, Bonacic-Koutecký V (1987) Phys Rev B 35:9437

    Google Scholar 

  11. Koutecký J, Fantucci P (1986) Z Phys D 3:147

    Google Scholar 

  12. Pacchioni G, Plavsic D, Koutecký J (1983) Ber Bunsenges Phys Chem 87:503

    Google Scholar 

  13. Plavsic D, Koutecký J, Pacchioni G, Bonacic-Koutecký V (1983) J Phys Chem 87:1096

    Google Scholar 

  14. Fantucci P, Koutecký J, Pacchioni G (1984) J Chem Phys 80: 325

    Google Scholar 

  15. McAdon MH, Goddard III WA (1985) Phys Rev Lett 55:2563; McAdon MH, Goddard III WA (1985) J Non Cryst Solids 75: 149; McAdon MH, Goddard III WA (1987) J Phys Chem 91:2607

    PubMed  Google Scholar 

  16. Koutecký J, Pacchioni G, Jeung GH, Hass EC (1985) Surf Sci 156:650

    Google Scholar 

  17. Schwarz WHE, Valtazanos P, Ruedenberg K (1985) Theor Chim Acta 68:471

    Google Scholar 

  18. Bader RFW, Nguyen-Dang TT (1981) Adv Quantum Chem 14:63

    Google Scholar 

  19. Bader RFW, Nguyen-Dang TT, Tal Y (1981) Rep Prog Phys (1981) 44:893;

    Google Scholar 

  20. Bader RFW, Essen H (1984) J Chem Phys 80:1943

    Google Scholar 

  21. Besnainou S, Roux M, Daudel R, Compt Rend (1955) 241:311

    Google Scholar 

  22. Beckmann HO, Koutecký J (1982) Surf Sci 120:127 and references therein

    Google Scholar 

  23. Clementi E, Corongiu G (1982) Chem Phys Lett 90:359. The geometrical basis set for Li [13s] has been augmented by a more contracted and a more diffuses function; the 2p and 3d exponents are the same of basisB andC. The corresponding energy of Li(2S), −7.4326766 au, has to be compared with the HF limit value −7.4327257 au (Clementi E, Roetti C (1974) At Data Nucl Data Tables 14:177)

    Google Scholar 

  24. Buenker RJ Peyerimhoff SD (1974) Theor Chim Acta 35:33

    Google Scholar 

  25. Buenker RJ, Peyerimhoff SD, Butscher W (1978) Mol Phys 35:771

    Google Scholar 

  26. Buenker RJ (1980) In: Burton PG (ed) Proceedings of the Workshop on Quantum Chemistry and Molecular Physic. Woollongong, Australia

  27. Buenker RJ (1982) Studies in physical and theoretical chemistry vol 21. Elsevier, Amsterdam

    Google Scholar 

  28. Buenker RJ, Phillip RA (1985) J Mol Struct 123:291

    Google Scholar 

  29. Biegler-König FW, Bader RFW, Tang T (1982) J Comput Chem 13:317;

    Google Scholar 

  30. An AIMPAC modified version for GOULD-SEL computers was actually used (Gatti C unpublished work)

  31. 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)

  32. 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 MS 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

  33. Bader RFW, Slee TS, Cremer D, Kraka E (1983) J Am Chem Soc 105:5061

    Google Scholar 

  34. Gatti C, Bader RFW, MacDougall PJJ: J Chem Phys, submitted;

  35. Dunning TH (1970) J Chem Phys 53:2823; thed exponent was taken from [16]

    Google Scholar 

  36. 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)

  37. Wiberg KB, Bader RFW, Lau CDH (1987) J Am Chem Soc 109:1001;

    Google Scholar 

  38. Bader RFW, Larouche A, Gatti C, Carroll MT, MacDougall PJ, Wiberg KB (1987) J Chem Phys 87:1142

    Google Scholar 

  39. 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

  40. Gatti C, Barzaghi M, Simonetta M (1985) J Am Chem Soc 107:878;

    Google Scholar 

  41. Simonetta M, Barzaghi M, Gatti C (1986) J Mol Struct 138:39

    Google Scholar 

  42. Wiberg KB, Bader RFW, Lau CDH (1987) J Am Chem Soc 109:985

    Google Scholar 

  43. 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]

  44. 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

  45. 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

  46. These arguments are thoroughly discussed by Bader RFW, MacDougall PJ, Lau CDH (1984) J Am Chem Soc 106:1594

    Google Scholar 

  47. Cremer D, Kraka E, (1984) Croat Chem Acta 57:1265

    Google Scholar 

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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

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