Abstract
The symmetric bissilyl-dione 3 reveals two well-separated n → π* absorption bands at λ(max) = 637 nm (ε = 140 mol(-1) dm(3) cm(-1)) and 317 nm (ε = 2460 mol(-1) dm(3) cm(-1)). Whereas excitation of 3 at λ = 360/365 nm affords an isolable siloxyketene 4 in excellent yields, irradiation at λ = 590/630 nm leads to the stereo-selective and quantitative formation of the siloxyrane 5. These remarkable wavelength-dependent rearrangements are based on the electronic and steric properties provided by the hypersilyl groups. While the siloxyketene 4 is formed via a hitherto unknown 1,3-hypersilyl migration via the population of a second excited singlet state (S(2), λ(max) = 317 nm, a rare case of anti-Kasha reactivity), the siloxyrane 5 emerges from the first excited triplet state (T(1)via S(1)λ(max) = 637 nm). These distinct reaction pathways can be traced back to specific energy differences between the S(2), S(1) and T(1), an electronic consequence of the bissilyl substited α-dione (the "pearl"). The hypersilyl groups act as protective ''oyster shell", which are responsible for the clean formation of 4 and 5 basically omitting side products. We describe novel synthetic pathways to achieve hypersilyl substitution (3) and report an in-depth investigation of the photorearrangements of 3 using UV/vis, in situ IR, NMR spectroscopy and theoretical calculations.