Abstract
Millimeter-sized single crystals of the title compound have been grown from a Sn-rich melt and neutron diffraction data recorded at room temperature and 20 K have been used to confirm and refine the crystal structure. The Ir3Ge7 structure-type, cubic Im3m can be viewed as a framework of alternating corner linked Ru6Sn8 capped-octahedral clusters and Ru2Sn4 flattened-octahedral clusters, such that the latter form their own three-dimensional sublattice. The Ru-Sn distances determined for Ru3Sn7 fall in the middle of the observed range tabulated from the handful of known Ru-Sn distances in intermetallics. The resistivity of Ru3Sn7 is metallic, with a value of 72 μΩ cm at 300 K and 0.5 μΩ cm at 5 K. The magnetic susceptibility is diamagnetic at room temperature, but becomes paramagnetic as the temperature is lowered. We interpret the susceptibility as being due to a diamagnetic 'core' contribution and a paramagnetic contribution arising from the Ru d orbitals.
Original language | English |
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Pages (from-to) | 157-159 |
Number of pages | 3 |
Journal | Journal of Alloys and Compounds |
Volume | 281 |
Issue number | 2 |
DOIs | |
State | Published - Dec 18 1998 |
Funding
Oak Ridge National Laboratory is managed by Lockheed Martin Energy Research Corporation for the U.S. Department of Energy under contract number DE-AC05-96OR22464.
Keywords
- Crystal structure
- Intermetallic
- Neutron diffraction
- Ruthenium stannide