[n.n.n]Propellanes and bicyclo[n.n.n]alkanes (1=n=3) in which the bridgeheads and bridges are composed of different Group 14 elements will not be ideal homologues of the all-carbon propellanes and bicycloalkanes. We used quantum-chemical calculations to conclude which of these could possibly be stable at ambient temperature. Structures, strain, and dimerization energies of [n.n.n]propellanes and bicyclo[n.n.n]alkanes with C-based tethers and with Si, Ge, or Sn at the bridgehead positions were calculated. The aptitude to add water was probed in selected cases. Comparisons were made with the analogous all-C propellanes and bicycloalkanes. All heavy 1,(n+2)-dimetallabicyclo[n.n.n]alkanes should be thermally stable and suitable synthetic targets, even though the moisture sensitivity of 1,3-dimetallabicyclo[1.1.1]pentanes increases as Group 14 is descended. For 1,(n+2)-dimetalla[n.n.n]propellanes, the incompatibility between the tether and M--M bond lengths impacts strongly on structure and stability. At ambient temperature 1,3-disila[1.1.1]propellanes should oligomerize instantly upon formation, whereas 1,3-digerma- and 1,3-distanna[1.1.1]propellanes should be less prone to oligomerize and possibly isolable. The 1,4-dimetalla[2.2.2]propellanes with M=Si-Sn have biradical ground states and can presumably only be observed under inert conditions at cryogenic temperatures. Finally, we predict that 1,5-disila[3.3.3]propellane will be persistent at ambient temperature, but 1,5-distanna[3.3.3]propellane should rapidly oligomerize.
We present a multistate complete active space second-order perturbation theory computational study aimed to predict the low-lying electronic excitations of four compounds that can be viewed as two disilane units connected through alkane bridges in a bicyclic cage. The analysis has focused on 1,4-disilyl-1,4-disilabicyclo[2.2.1]heptane (1a), 1,4-bis(trimethylsilyl)-1,4-disilabicyclo[2.2.1]heptane (1b), 1,4-disilyl-1,4-disilabicyclo[2.1.1]hexane (2a), and 1,4-bis(trimethylsilyl)-1,4-disilabicyclo[2.1.1]hexane (2b). The aim has been to find out the nature of the lowest excitations with significant oscillator strengths and to investigate how the cage size affects the excitation energies and the strengths of the transitions. Two different substituents on the terminal silicon atoms (H and CH3) were used in order to investigate the end group effects. The calculations show that the lowest allowed excitations are of the same character as that found in disilanes but now red-shifted. As the cage size is reduced from a 1,4-disilabicyclo[2.2.1]heptane to a 1,4-disilabicyclo[2.1.1]hexane, the Si...Si through-space distance decreases from approximately 2.70 to 2.50 A and the lowest allowed transitions are red-shifted by up to 0.9 eV, indicating increased interaction between the two Si-Si bonds. The first ionization potential, which corresponds to ionization from the Si-Si sigma orbitals, is lower in 1b and 2b than in Si2Me6 by approximately 0.9 and 1.2 eV, respectively. Moreover, 1b and 2b, which have methyl substituents at the terminal Si atoms, have slightly lower excitation energies than the analogous species 1a and 2a.
The strain energies and through-space distances between the two bridgehead E atoms of a selection of 1,3-dimethyl-1,3-ditetrelbicyclo[1.1.1]pentanes (tetrel E = Si, Ge or Sn) were examined by quantum chemical calculations at MP2 and B3LYP levels. The aim is to identify which bridges lead to short through-space E,E distances, and simultaneously, to as low strain as possible. A short E,E distance should improve through-space interaction, and a low strain should promote the thermal stability and possibly also facilitate their synthesis. The bridges examined included CH 2 , CMe 2 , CtBu 2 , C(CH 2 ) n (n = 2-4), O, NMe, S, PMe, SiMe 2 , GeMe 2 , and SnMe 2 . The calculations indicate that the phospha bridge is a good compromise providing reasonably low strain as well as E,E through-space distances which are only longer than normal E E single bonds by factors of 1.06-1.10.
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