Disiloxane has a simple structure that consists of a
siloxane bond (Si−O−Si) and hydrogen R groups. The structure of disiloxane has been studied by a variety of spectroscopic methods such as
electron diffraction,
X-ray crystallography, For example, in the solid state at a temperature of 108 K, disiloxane itself has an Si−O−Si bond angle of 142°. In contrast, the C−O−C bond angle in the carbon analogue of disiloxane,
dimethyl ether, is 111°. The unusual bond angle in disiloxane has been attributed primarily to negative
hyperconjugation between oxygen
p orbitals and silicon–carbon
σ* antibonding orbitals,
p(O) → σ*(Si−R), a form of
π backbonding. A secondary and much smaller contribution to the
silicon–oxygen bond in disiloxanes involves π backbonding from oxygen 2
p orbitals to silicon 3
d orbitals,
p(O) →
d(Si). Because of this interaction, the Si−O bonds can exhibit some partial double bond behavior and the oxygen atoms are much less
basic than in the carbon analogue, dimethyl ether. In addition to studies of bond angles, vibrational analyses have also been done to determine the symmetry elements of disiloxane. IR and Raman spectroscopy have been used to propose a point group of D3d. While disiloxane itself has a
bent molecular geometry at oxygen, the related compound hexaphenyldisiloxane, Ph3Si−O−SiPh3, has an Si−O−Si angle of 180°. == Synthesis ==