The extent and depth of the so-called boron connection suggested recently by the present author [J. Chem. Phys. 128, 184305 (2008)] for the Si(n-2)C(2)H(2)-C(2)B(n-2)H(n) isovalent species [following similar connection of (Si(n))(2-)-(B(n)H(n))(2-) dianions] are further investigated by considering larger species up to n=12 and additional isovalent moieties. Here we consider, using density functional and coupled clusters theory, isovalent Si(n-2)C(2)H(2) and Ge(n-2)C(2)H(2) clusters, in comparison to the corresponding C(2)B(n-2)H(n) carboranes and to each other for n=3-8, 12. Special attention is given to the n=8 species, where the corresponding carborane is highly fluxional, and to n=12, where the "parent structures" of the corresponding (Si(12))(2-) and (B(12)H(12))(2-) dianions have drastically different symmetries. The structures generated by substitutions on (Si(12))(2-), as well as (B(12)H(12))(2-), are compared and interrelated for both C(2)B(10)H(12) and Si(10)C(2)H(12). The carborane generated from the C(s) (Si(12))(2-) dianion provides an illustrative example of carborane rearrangements, reverting after geometry optimization to the second lowest C(2)B(10)H(12) meta isomer of C(2v) symmetry, 0.12 eV above the lowest energy para isomer. This demonstrates the amphidirectional character of the boron connection. It is found that n=8 is the upper limit of the n range in which the isolobal Si(n-2)C(2)H(2)-C(2)B(n-2)H(n) analogy is fully operative not only for the lowest but also for the second and third lowest energy states. For n
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http://dx.doi.org/10.1063/1.3071260 | DOI Listing |
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