Henryite [(Ag$_{1.48}$Cu$_{1.44}$Fe$_{0.32}$)Te$_{2}$] Structure: AB3C2_cP12_224_a_d_b-001

Picture of Structure; Click for Big Picture
Prototype (Ag$_{1.48}$Cu$_{1.44}$Fe$_{0.32}$)Te$_{2}$
AFLOW prototype label AB3C2_cP12_224_a_d_b-001
Mineral name henryite
ICSD 239361
CCDC 1710367
Pearson symbol cP12
Space group number 224
Space group symbol $Pn\overline{3}m$
AFLOW prototype command aflow --proto=AB3C2_cP12_224_a_d_b-001
--params=$a$

  • The ICSD entries for (Bindi, 2014, ICSD 23936) and (Cohen-Addad, 1971 ICSD 5165) are identical except for the rounding of the site occupation. We reference the newer version as it is more accessible to the user.
  • The (2a) and (6d) sites are 37% silver, 48% copper, and 0.8% iron, giving the observed stoichiometry.
  • We arbitrarily assign silver to the (2a) site and copper to the (6c) cite.
  • Both papers put the structure in space group $Fd\overline{3}c$ #228, with the atoms occupying the (16a), (32c), and (48d) sites, however these sites are identical to the (2a), (4b) and (6d) sites of space group $Pn\overline{3}m$ #224 with $a_{224} = 1/2 a_{228}$. AFLOW favors the smaller unit cell, so we assign this structure to space group #224.
  • In addtion, if the (2a) and (6c) sites are fully alloyed, this becomes the fluorite ($C1$) structure.
  • The reported structure can be viewed by clicking the load block button and entering a value of 12.2\,Ångström.

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

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) Ag 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) Ag I
$\mathbf{B_{3}}$ = $0$ = $0$ (4b) Te 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) Te 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) Te 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) Te I
$\mathbf{B_{7}}$ = $\frac{1}{4} \, \mathbf{a}_{1}+\frac{3}{4} \, \mathbf{a}_{2}+\frac{3}{4} \, \mathbf{a}_{3}$ = $\frac{1}{4}a \,\mathbf{\hat{x}}+\frac{3}{4}a \,\mathbf{\hat{y}}+\frac{3}{4}a \,\mathbf{\hat{z}}$ (6d) Cu I
$\mathbf{B_{8}}$ = $\frac{3}{4} \, \mathbf{a}_{1}+\frac{1}{4} \, \mathbf{a}_{2}+\frac{3}{4} \, \mathbf{a}_{3}$ = $\frac{3}{4}a \,\mathbf{\hat{x}}+\frac{1}{4}a \,\mathbf{\hat{y}}+\frac{3}{4}a \,\mathbf{\hat{z}}$ (6d) Cu I
$\mathbf{B_{9}}$ = $\frac{3}{4} \, \mathbf{a}_{1}+\frac{3}{4} \, \mathbf{a}_{2}+\frac{1}{4} \, \mathbf{a}_{3}$ = $\frac{3}{4}a \,\mathbf{\hat{x}}+\frac{3}{4}a \,\mathbf{\hat{y}}+\frac{1}{4}a \,\mathbf{\hat{z}}$ (6d) Cu I
$\mathbf{B_{10}}$ = $\frac{1}{4} \, \mathbf{a}_{1}+\frac{3}{4} \, \mathbf{a}_{2}+\frac{1}{4} \, \mathbf{a}_{3}$ = $\frac{1}{4}a \,\mathbf{\hat{x}}+\frac{3}{4}a \,\mathbf{\hat{y}}+\frac{1}{4}a \,\mathbf{\hat{z}}$ (6d) Cu I
$\mathbf{B_{11}}$ = $\frac{3}{4} \, \mathbf{a}_{1}+\frac{1}{4} \, \mathbf{a}_{2}+\frac{1}{4} \, \mathbf{a}_{3}$ = $\frac{3}{4}a \,\mathbf{\hat{x}}+\frac{1}{4}a \,\mathbf{\hat{y}}+\frac{1}{4}a \,\mathbf{\hat{z}}$ (6d) Cu I
$\mathbf{B_{12}}$ = $\frac{1}{4} \, \mathbf{a}_{1}+\frac{1}{4} \, \mathbf{a}_{2}+\frac{3}{4} \, \mathbf{a}_{3}$ = $\frac{1}{4}a \,\mathbf{\hat{x}}+\frac{1}{4}a \,\mathbf{\hat{y}}+\frac{3}{4}a \,\mathbf{\hat{z}}$ (6d) Cu I

References

  • L. Bindi, Chemical and structural characterization of henryite, (Cu,Ag)$_{3+x}$Te$_{2}$ (x ≈ 0.40): A new structure type in the (Ag)-Cu-Te system, Solid State Sciences 38, 108–111 (2014), doi:10.1016/j.solidstatesciences.2014.10.008.
  • C. Cohen-Addad, Etude du compose Te (O H)6 par diffraction des neutrons, Bull. Soc. Franc. Mineral. Cristall. 94, 172–174 (1971).

First cited in

  • N. Anderson, M. J. Mehl, H. Eckert, S. Divilov, X. Campilongo, S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 5. Submitted to Computational Materials Science (2026).

Geometry files


Prototype Generator

aflow --proto=AB3C2_cP12_224_a_d_b --params=$a$

Species:

Running:

Output: