Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: AB3_oC8_65_a_bf-001

This structure originally had the label AB3_oC8_65_a_bf. 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/JBK1
or https://aflow.org/p/AB3_oC8_65_a_bf-001
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CdPt$_{3}$ (New $L1_{3}$) Structure: AB3_oC8_65_a_bf-001

Picture of Structure; Click for Big Picture
Prototype CdPt$_{3}$
AFLOW prototype label AB3_oC8_65_a_bf-001
Strukturbericht designation $L1_{3}$
ICSD none
Pearson symbol oC8
Space group number 65
Space group symbol $Cmmm$
AFLOW prototype command aflow --proto=AB3_oC8_65_a_bf-001
--params=$a, \allowbreak b/a, \allowbreak c/a$

  • This is not the $L1_{3}$ CuPt structure labeled by (Ewald, 1931) as $L1_{3}$. That structure is now considered obsolete.
  • This structure has not been experimentally confirmed, but it has frequently been predicted as a low energy structure. (Hart, 2009) has a review of these calculations. It was originally given the $L1_{3}$ designation. As this has been frequently used in the literature ( e.g. Mehl, 2017), we will continue to used it despite the possible confusion.
  • Data for this structure comes from the supplemental material of (Hart, 2013).

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

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $0$ = $0$ (2a) Cd I
$\mathbf{B_{2}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}$ (2b) Pt I
$\mathbf{B_{3}}$ = $\frac{1}{2} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{4}a \,\mathbf{\hat{x}}+\frac{1}{4}b \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}$ (4f) Pt II
$\mathbf{B_{4}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{4}a \,\mathbf{\hat{x}}- \frac{1}{4}b \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}$ (4f) Pt II

References

  • G. L. W. Hart, Verifying predictions of the L1$_3$ crystal structure in Cd-Pt and Pd-Pt by exhaustive enumeration, Phys. Rev. B 80, 014106 (2009), doi:10.1103/PhysRevB.80.014106.
  • G. L. W. Hart, S. Curtarolo, T. B. Massalski, and O. Levy, Comprehensive Search for New Phases and Compounds in Binary Alloy Systems Based on Platinum-Group Metals, Using a Computational First-Principles Approach, Phys. Rev. X 3, 041305 (2013), doi:10.1103/PhysRevX.3.041035.
  • P. P. Ewald and C. Hermann, eds., Strukturbericht 1913-1928 (Akademische Verlagsgesellschaft M. B. H., Leipzig, 1931).
  • M. J. Mehl, D. Hicks, C. Toher, O. Levy, R. M. Hanson, G. Hart, and S. Curtarolo, The AFLOW library of crystallographic prototypes: part 1, Comp. Mater. Sci. 136, S1–S828 (2017), doi:10.1016/j.commatsci.2017.01.017.

Prototype Generator

aflow --proto=AB3_oC8_65_a_bf --params=$a,b/a,c/a$

Species:

Running:

Output: