An idealized model for the crystal structure of intermetallic compounds isostructural with Mg3Cr2Al18.

Mg3Cr2Al18 (abbreviated in this report as MCA) is the parent phase for a large class of intermetallic compounds that belong to the cubic crystal space group, $Fd\bar{3}m$ Fd 3 ¯ m. The purpose of this paper is to introduce an ideal, unrelaxed crystal structure for compounds isostructural with MCA. There are five distinct atomic sublattices in MCA compounds, which can be denoted, A, B, C, D, and E. With this, a general description for MCA structures can be written as $A_1^{8a} B_2^{16c} C_2^{16d} D_6^{48f} E_{12}^{96g}$ A 1 8 a B 2 16 c C 2 16 d D 6 48 f E 12 96 g , where the superscripts represent the Wyckoff special equipoints associated with the various sublattices in MCA, and the subscripts indicate the contributions of each sublattice to the stoichiometry of one formula unit in an any given MCA-structured compound. Sublattices D and E are where deviations from ideality occur in real, MCA-like compounds. This paper examines MCA bond lengths, nearest-neighbour polyhedral arrangements, 3-D sublattice crystal structures, 2-D atom tessellation patterns, and crystal chemical effects associated with atomic relaxations on the D and E sublattices. The ideal MCA crystal structure developed in this report provides an appropriate initial structure for use as input to crystal structure refinements of diffraction data for MCA-like phases being examined experimentally, or as input for computational, atomistic simulations of the structures of such compounds. [ABSTRACT FROM AUTHOR]