Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
1627296 | Journal of Alloys and Compounds | 2006 | 5 Pages |
Abstract
The crystal structures of the R3Mg0.5GeS7 (R = Y, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Ho and Er) compounds (La3CuSiS7 structure type, space group P63, Pearson symbol hP23) were determined by means of X-ray powder diffraction: a = 0.9788(1) nm, c = 0.57745(5) nm, RBragg = 0.0814 (Y3Mg0.5GeS7); a = 1.0262(2) nm, c = 0.57849(7) nm, RBragg = 0.0687 (Ce3Mg0.5GeS7); a = 1.01249(3) nm, c = 0.58040(2) nm, RBragg = 0.0832 (Pr3Mg0.5GeS7); a = 1.00701(3) nm, c = 0.58047(3) nm, RBragg = 0.0636 (Nd3Mg0.5GeS7); a = 0.99500(3) nm, c = 0.57872(3) nm, RBragg = 0.0870 (Sm3Mg0.5GeS7); a = 0.99319(3) nm, c = 0.57083(3) nm, RBragg = 0.0901 (Gd3Mg0.5GeS7); a = 0.98007(5) nm, c = 0.57843(4) nm, RBragg = 0.0859 (Tb3Mg0.5GeS7); a = 0.97698(4) nm, c = 0.57675(5) nm, RBragg = 0.0931 (Dy3Mg0.5GeS7); a = 0.9735(2) nm, c = 0.57941(7) nm, RBragg = 0.0763 (Ho3Mg0.5GeS7); a = 0.9694(2) nm, c = 0.57994(7) nm, RBragg = 0.0724 (Er3Mg0.5GeS7). The R-centered trigonal prisms, Mg-centered octahedra and Ge-centered tetrahedra can be selected in the crystal structure of the R3Mg0.5GeS7 compounds.
Related Topics
Physical Sciences and Engineering
Materials Science
Metals and Alloys
Authors
M.R. Huch, L.D. Gulay, I.D. Olekseyuk,