Re. Dinnebier et al., Bulk modulus and high-pressure crystal structures of tetrakis(trimethylsilyl)methane C[Si(CH3)(3)](4) determined by X-ray powder diffraction, ACT CRYST B, 56, 2000, pp. 310-316
The pressure dependence of the crystal structure of cubic tetrakis(trimethy
lsilyl)methane C[Si(CH3)(3)](4) (TC) (P < 16.0 GPa, T = 298 K) is reported
using high-resolution angle-dispersive X-ray powder diffraction. The compou
nd has crystal structures with the molecules in a cubic-close-packed (c.c.p
.) arrangement. It shows three phase transitions in the measured pressure r
ange. At ambient conditions, TC has space group Fm (3) over bar m (Z = 4) w
ith a = 12.8902 (2) Angstrom, V = 2141.8 (1) Angstrom(3) (phase I). Between
0 and 0.13 GPa TC exhibits a first-order phase transition into a structure
with space group Pa (3) over bar (phase II). A second first-order phase tr
ansition occurs between 0.2 and 0.28 GPa into a structure with space group
P2(1)3 (phase III). Under non-hydrostatic pressure conditions (P > 10 GPa)
a transformation is observed into a c.c.p. structure that is different from
the face-centred-cubic structure at ambient conditions. A non-linear compr
ession behaviour is observed, which could be described by a Vinet relation
in the range 0.28-4.8 GPa. The extrapolated bulk modulus of the high-pressu
re phase III was determined to be K-o = 7.1(8)GPa. The crystal structures i
n phase III are refined against X-ray powder data measured at several press
ures between 0.49 and 4.8 GPa, and the molecules are found to be fully orde
red. This is interpreted to result from steric interactions between neighbo
uring molecules, as shown by analysing the pressure dependence of intramole
cular angles, torsion angles and intermolecular distances. Except for their
cell dimensions, phases I, II and III are found to be isostructural to the
corresponding phases at low temperatures.