Zdetsis Aristides D
Department of Physics, University of Patras, GR-26500 Patras, Greece.
J Chem Phys. 2009 Feb 14;130(6):064303. doi: 10.1063/1.3071260.
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<or=8 all three pairs of structures are isovalent, isostructural, and isolobal. For large values of n (n>8) the boron connection, although not fully isolobal, is still valid in a broader and more general sense, still providing deeper and broader fundamental understanding and insight for both species. It was also found that the Ge(n-2)C(2)H(2) clusters are not fully homologous (isolobal) neither to the isovalent Si(n-2)C(2)H(2) clusters nor to the corresponding C(2)B(n-2)H(n) carboranes, preferring structures in which the two carbon atoms are always in adjacent positions. This is attributed to the relative weakness of the Ge-Ge and Ge-C bonds relative to Si-Si and Si-C bonds and the "inert pair effect."
作者[《化学物理杂志》128, 184305 (2008)]最近提出的Si(n - 2)C₂H₂ - C₂B(n - 2)Hₙ等价物种[继(Siₙ)²⁻ - (BₙHₙ)²⁻二价阴离子的类似连接之后]的所谓硼连接的范围和深度,通过考虑直至n = 12的更大物种和额外的等价部分进一步进行了研究。在这里,我们使用密度泛函和耦合簇理论,考虑等价的Si(n - 2)C₂H₂和Ge(n - 2)C₂H₂簇,与相应的C₂B(n - 2)Hₙ碳硼烷以及n = 3 - 8、12时彼此进行比较。特别关注n = 8的物种,其中相应的碳硼烷具有高度的流动性,以及n = 12的物种,其中相应的(Si₁₂)²⁻和(B₁₂H₁₂)²⁻二价阴离子的“母体结构”具有截然不同的对称性。比较并关联了在(Si₁₂)²⁻以及(B₁₂H₁₂)²⁻上进行取代所产生的结构,对于C₂B₁₀H₁₂和Si₁₀C₂H₁₂都是如此。由Cₛ (Si₁₂)²⁻二价阴离子生成的碳硼烷提供了一个碳硼烷重排的示例,在几何优化后恢复为C₂B₁₀H₁₂的第二低能量的C₂ᵥ对称间位异构体,比最低能量的对位异构体高0.12 eV。这证明了硼连接的双向性。发现n = 8是n范围中的上限,在该范围内,等叶Si(n - 2)C₂H₂ - C₂B(n - 2)Hₙ类比不仅对于最低能量状态,而且对于第二和第三低能量状态都完全有效。对于n≤8,所有三对结构都是等价、同结构且等叶的。对于n的较大值(n > 8),硼连接虽然不完全等叶,但在更广泛和更一般的意义上仍然有效,仍然为这两种物种提供了更深入和更广泛的基本理解和见解。还发现Ge(n - 2)C₂H₂簇既不完全与等价的Si(n - 2)C₂H₂簇同源(等叶),也不完全与相应的C₂B(n - 2)Hₙ碳硼烷同源,更倾向于两个碳原子总是处于相邻位置的结构。这归因于相对于Si - Si和Si - C键,Ge - Ge和Ge - C键的相对较弱以及“惰性电子对效应”。