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Carim, A. H.,1,2
Dera, P., 1
Finger, Larry W.1
Mysen, Bjorn O.1
Prewitt, Charles T.1 and Schlom, D. G.2
1 Geophysical
Laboratory and Center for High-pressure Research, 5251 Broad
Branch Rd., NW, Washington, DC 20015-1305, USA
2 Dept.
Mater. Sci. and Engin., The Pennsylvania State University, University
Park, PA 16802, USA
Geophysical Laboratory,
5251 Broad Branch Rd., NW
Washington DC 20015-1305, USA
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Abstract
The crystal structure of Ba4Ru3O10
has been determined by single-crystal x-ray diffraction at room
pressure. F refinements to R-0.0203 at room temperature and ambient
pressure, the material is orthorhombic with space group Cmca
(S-ace group no. 64) and has lattice parameters of a=5.7762 (15)Å,
b=13.271 (4)Å, and c=13.083 (3)Å. The unit cell thus
has a volume of V=1002.9(8)Å3 and contains four formula
units (Z=4). Ba4Ru3O10 is therefore of higher symmetry than the
previously reported monoclinic structure based on powder x-ray
data. It is isostructural with the quaternary oxides Ba4(Ti,Pt)3O10
and Ba4Ir2AlO10 and the ternay fluorides Cs=4M3F10 (M=Mg, Co,
Ni, Zn). Kinked chains of RuO6 octahedra run along the c direction,
consisting of sets of three face-sharing units joined at the
corners of the end-units to additional similar sets. The two
distinct Ba sites show 10-fold and 11-fold coordination.
Compressibilities and bulk
modulus have been determined from lattice parameter variations
at pressures up to 5.4 GPa. No phase transition was upserved
up to this pressure. Compressibility is greatest along the c
axis and the bulk modulus from a weighted fit to a Vinte equation
of state is 113.3(47) GPa.
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