An ideal cubic perovskite structure is obtained by putting La at the cube corners, Re at the body center, and N at the face centers. In fractional crystal coordinates one convenient basis is
The counting is La, one Re and N per cell. Corner-sharing octahedra form the network, with La in the larger interstices. The ideal cell illustrates the connectivity; octahedral tilting can lower the actual crystal symmetry.
Figure 1.
Ideal perovskite connectivity for lanthanum rhenium nitride
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