Abstract
Using the generalized valence bond (GVB) method, we have examined the bonding in numerous small clusters of Li atoms (Lin and Lin+, n ≤ 13). Our conclusion is that the optimum bonding involves interstitially localized singly occupied orbitals, e.g., (1) bond-centered orbitals for one-dimensional clusters (e.g., rings such as Li4, Li6, Li8, and Li10 and linear chains such as Li3+, Cu3+, Li8+, Li8, Li8-, and Li13+), (2) equilateral-triangle-centered orbitals for planar close-packed clusters (e.g., Li10, Li124+, and Li13+), and (3) tetrahedron-centered orbitals for three-dimensional clusters (examples here include three high-symmetry [icosahedral (Ih), face-centered cubic (fcc), and hexagonal close-packed (hcp)] Li13+ structures and three low symmetry [γ-brass-like] Li13+ structures. Of the three high symmetry Li13+ clusters, Ih has the lowest energy while total energies for fcc and hcp are 0.26 and 0.56 eV higher, respectively. GVB wave functions for these three clusters suggest a set of rules predicting structures even more stable than the icosahedron. These lower energy structures [denoted as OPTET (optimum tetrahedral)] maximize the number of tetrahedra under the restrictions of the rules (e.g. minimizing the number of occupied tetrahedra sharing corners) and lead to relatively low symmetry, e.g. C2v, Cs. These OPTET clusters coincide with truncations of the γ-brass structure. The lowest energy Li13+ OPTET cluster [γ-(4,4,5), C2v] has a total energy 0.58 eV lower than that of the icosahedron. Suggestions are given on the relevance of these results for stability and reactivity of small clusters and on the extension of these ideas to infinite systems.
| Original language | English |
|---|---|
| Pages (from-to) | 2607-2626 |
| Number of pages | 20 |
| Journal | Journal of Physical Chemistry |
| Volume | 91 |
| Issue number | 10 |
| DOIs | |
| Publication status | Published - 1 Jan 1987 |
| Externally published | Yes |
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