Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: A2B_cP6_224_b_a-001

This structure originally had the label A2B_cP6_224_b_a. 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/WUJH
or https://aflow.org/p/A2B_cP6_224_b_a-001
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Cuprite (Cu$_{2}$O, $C3$) Structure: A2B_cP6_224_b_a-001

Picture of Structure; Click for Big Picture
Prototype Cu$_{2}$O
AFLOW prototype label A2B_cP6_224_b_a-001
Strukturbericht designation $C3$
Mineral name cuprite
ICSD 52043
Pearson symbol cP6
Space group number 224
Space group symbol $Pn\overline{3}m$
AFLOW prototype command aflow --proto=A2B_cP6_224_b_a-001
--params=$a$

Other compounds with this structure

Ag$_{2}$O,  Pb$_{2}$O


  • (Restori, 1986) gives the equilibrium lattice constant of Cu$_{2}$O as $a$=4.627Å, but gives nearest-neighbor distances which yield a lattice constant of 4.267Å. Since this value agrees with other sources, including those in (Downs, 2003), we use it. The ICSD entry uses 4.2685Å.

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

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $\frac{1}{4} \, \mathbf{a}_{1}+\frac{1}{4} \, \mathbf{a}_{2}+\frac{1}{4} \, \mathbf{a}_{3}$ = $\frac{1}{4}a \,\mathbf{\hat{x}}+\frac{1}{4}a \,\mathbf{\hat{y}}+\frac{1}{4}a \,\mathbf{\hat{z}}$ (2a) O I
$\mathbf{B_{2}}$ = $\frac{3}{4} \, \mathbf{a}_{1}+\frac{3}{4} \, \mathbf{a}_{2}+\frac{3}{4} \, \mathbf{a}_{3}$ = $\frac{3}{4}a \,\mathbf{\hat{x}}+\frac{3}{4}a \,\mathbf{\hat{y}}+\frac{3}{4}a \,\mathbf{\hat{z}}$ (2a) O I
$\mathbf{B_{3}}$ = $0$ = $0$ (4b) Cu I
$\mathbf{B_{4}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}a \,\mathbf{\hat{y}}$ (4b) Cu I
$\mathbf{B_{5}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}a \,\mathbf{\hat{z}}$ (4b) Cu I
$\mathbf{B_{6}}$ = $\frac{1}{2} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{y}}+\frac{1}{2}a \,\mathbf{\hat{z}}$ (4b) Cu I

References

  • R. Restori and D. Schwarzenbach, Charge Density in Cuprite, Cu$_2$O, Acta Crystallogr. Sect. B 42, 201–208 (1986), doi:10.1107/S0108768186098336.
  • R. T. Downs and M. Hall-Wallace, The American Mineralogist Crystal Structure Database, Am. Mineral. 88, 247–250 (2003).

Found in

  • A. Kirfel and K. Eichhorn, Accurate structure analysis with synchrotron radiation. The electron density in Al$_2$O$_3$ and Cu$_2$O, Acta Crystallogr. Sect. A 46, 271–284 (1990), doi:10.1107/S0108767389012596.

Prototype Generator

aflow --proto=A2B_cP6_224_b_a --params=$a$

Species:

Running:

Output: