Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: AB_hR2_166_a_b-001

This structure originally had the label AB_hR2_166_a_b. Calls to that address will be redirected here.

If you are using this page, please cite:
M. J. Mehl, D. Hicks, C. Toher, O. Levy, R. M. Hanson, G. L. W. Hart, and S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 1, Comp. Mat. Sci. 136, S1-S828 (2017). (doi=10.1016/j.commatsci.2017.01.017)

Links to this page

https://aflow.org/p/3A9R
or https://aflow.org/p/AB_hR2_166_a_b-001
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Rhombohedral CuPt ($L1_{1}$) Structure: AB_hR2_166_a_b-001

Picture of Structure; Click for Big Picture
Prototype CuPt
AFLOW prototype label AB_hR2_166_a_b-001
Strukturbericht designation $L1_{1}$
ICSD 107118
Pearson symbol hR2
Space group number 166
Space group symbol $R\overline{3}m$
AFLOW prototype command aflow --proto=AB_hR2_166_a_b-001
--params=$a, \allowbreak c/a$

  • (Johansson, 1929) described two possible structures for CuPt. (Ewald, 1929) and later (Villars, 2007) used the description to determine the space group and atomic positions. This page describes the rhombohedral structure, which (Ewald, 1929) labeled Strukturbericht $L1_{1}$. The other structure is cubic, and was listed as $L1_{3}$.
  • (Barrett, 1980) noted that even slight additions of platinum above stoichiometry will cause a change in the crystal structure.
  • CuPt and KSH have the same AFLOW prototype label, AB_hR2_166_a_b. They are generated by the same symmetry operations with different sets of parameters (--params) specified in their corresponding CIF files.
  • This structure is given in the rhombohedral setting of space group $R\overline{3}m$ #166. The hexagonal setting may be obtained by adding --hex to the aflow command.

\[ \begin{array}{ccc} \mathbf{a_{1}}&=&\frac{1}{2}a \,\mathbf{\hat{x}}- \frac{\sqrt{3}}{6}a \,\mathbf{\hat{y}}+\frac{1}{3}c \,\mathbf{\hat{z}}\\\mathbf{a_{2}}&=&\frac{1}{\sqrt{3}}a \,\mathbf{\hat{y}}+\frac{1}{3}c \,\mathbf{\hat{z}}\\\mathbf{a_{3}}&=&- \frac{1}{2}a \,\mathbf{\hat{x}}- \frac{\sqrt{3}}{6}a \,\mathbf{\hat{y}}+\frac{1}{3}c \,\mathbf{\hat{z}} \end{array}\]

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $0$ = $0$ (1a) Cu I
$\mathbf{B_{2}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}c \,\mathbf{\hat{z}}$ (1b) Pt I

References

  • C. H. Johansson and J. O. Linde, Gitterstruktur und elektrisches Leitvermögen der Mischkristallreihen Au-Cu, Pd-Cu und Pt-Cu, Annalen der Physik 82, 449–478 (1927), doi:10.1002/andp.19273870402.
  • C. Barrett and T. B. Massalski, Structure of Metals – Crystallographic Methods, Principles, and Data (Pergammon Press, Oxford, New York, 1980).

Found in

  • P. P. Ewald and C. Hermann, eds., Strukturbericht 1913-1928 (Akademische Verlagsgesellschaft M. B. H., Leipzig, 1931).
  • P. Villars, K. Cenzual, J. Daams, R. Gladyshevskii, O. Shcherban, V. Dubenskyy, N. Melnichenko-Koblyuk, O. Pavlyuk, I. Savysyuk, S. Stoyko, and L. Sysa, Structure Types. Part 5: Space Groups (173) P63- (166) R-3m $\cdot$ CuPt: Datasheet from Landolt-Börnstein - Group III Condensed Matter $\cdot$ Volume 43A5: Structure Types. Part 5: Space Groups (173) P63 - (166) R-3m in SpringerMaterials, doi:10.1007/978-3-540-46933-9_359. Copyright 2007 Springer-Verlag.

Prototype Generator

aflow --proto=AB_hR2_166_a_b --params=$a,c/a$

Species:

Running:

Output: