The crystal structure of Na3ScF6 was investigated by high-pressure sin
gle-crystal X-rag diffraction techniques in the range from ambient con
ditions to 68.2 kbar, Pressure was measured by the ruby fluorescence m
ethod, The single-crystal structure determination at 27.9 kbar resulte
d in the cell parameters a = 5.484(1) Angstrom, b = 5.732(1) Angstrom,
c = 7.948(2) Angstrom, and beta = 90.96(3)degrees and the same space
group symmetry, P2(1)/n (Z = 2), as at ambient conditions, The 19 stru
ctural parameters needed to describe a model with isotropic displaceme
nt parameters were refined by least-squares techniques, For the 143 mo
st significant observed unique reflection amplitudes, the R value beca
me 0.047, When the pressure was increased from ambient to 27.9 kbar, t
he change in the geometry and the relative change in the volume of the
coordination polyhedron around the six-coordinated Sc3+ ion were negl
igible, Significant changes of the coordination volumes around the Na ions were observed, The volume decreases for the six-coordinated and
the eight-coordinated Na+ ions were similar, viz., 7 and 8%, The layer
ed stacking of the larger, low-charged F- and Na+ ions along [103] off
ers an explanation for the pattern which determines the changes of the
unit cell parameters with pressure, The relative change in unit cell
volume versus pressure in the range from ambient to 68.2 kbar was fit
to the Birch type equation of state, The isothermal bulk modulus at am
bient pressure and its pressure derivative were determined to be B-0 =
46.0(7) GPa and B-0' = 3.3(2), respectively. (C) 1998 Academic Press.