Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: A4B3_hR7_166_2c_ac-001

This structure originally had the label A4B3_hR7_166_2c_ac. Calls to that address will be redirected here.

If you are using this page, please cite:
D. Hicks, M. J. Mehl, E. Gossett, C. Toher, O. Levy, R. M. Hanson, G. L. W. Hart, and S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 2, Comp. Mat. Sci. 161, S1-S1011 (2019). (doi=10.1016/j.commatsci.2018.10.043)

Links to this page

https://aflow.org/p/YAHB
or https://aflow.org/p/A4B3_hR7_166_2c_ac-001
or PDF Version

Al$_{4}$C$_{3}$ ($D7_{1}$) Structure: A4B3_hR7_166_2c_ac-001

Picture of Structure; Click for Big Picture
Prototype Al$_{4}$C$_{3}$
AFLOW prototype label A4B3_hR7_166_2c_ac-001
Strukturbericht designation $D7_{1}$
ICSD 66751
Pearson symbol hR7
Space group number 166
Space group symbol $R\overline{3}m$
AFLOW prototype command aflow --proto=A4B3_hR7_166_2c_ac-001
--params=$a, \allowbreak c/a, \allowbreak x_{2}, \allowbreak x_{3}, \allowbreak x_{4}$

Other compounds with this structure

Th$_{3}$N$_{4}$


  • Al$_{4}$C$_{3}$ ($D7_{1}$) and Bi$_{4}$Te$_{3}$ have the same AFLOW prototype label, A4B3_hR7_166_2c_ac. They are generated by the same symmetry operations with different sets of parameters (--params) specified in their corresponding CIF files.

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

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $0$ = $0$ (1a) C I
$\mathbf{B_{2}}$ = $x_{2} \, \mathbf{a}_{1}+x_{2} \, \mathbf{a}_{2}+x_{2} \, \mathbf{a}_{3}$ = $c x_{2} \,\mathbf{\hat{z}}$ (2c) Al I
$\mathbf{B_{3}}$ = $- x_{2} \, \mathbf{a}_{1}- x_{2} \, \mathbf{a}_{2}- x_{2} \, \mathbf{a}_{3}$ = $- c x_{2} \,\mathbf{\hat{z}}$ (2c) Al I
$\mathbf{B_{4}}$ = $x_{3} \, \mathbf{a}_{1}+x_{3} \, \mathbf{a}_{2}+x_{3} \, \mathbf{a}_{3}$ = $c x_{3} \,\mathbf{\hat{z}}$ (2c) Al II
$\mathbf{B_{5}}$ = $- x_{3} \, \mathbf{a}_{1}- x_{3} \, \mathbf{a}_{2}- x_{3} \, \mathbf{a}_{3}$ = $- c x_{3} \,\mathbf{\hat{z}}$ (2c) Al II
$\mathbf{B_{6}}$ = $x_{4} \, \mathbf{a}_{1}+x_{4} \, \mathbf{a}_{2}+x_{4} \, \mathbf{a}_{3}$ = $c x_{4} \,\mathbf{\hat{z}}$ (2c) C II
$\mathbf{B_{7}}$ = $- x_{4} \, \mathbf{a}_{1}- x_{4} \, \mathbf{a}_{2}- x_{4} \, \mathbf{a}_{3}$ = $- c x_{4} \,\mathbf{\hat{z}}$ (2c) C II

References

  • T. M. Gesing and W. Jeitschko, The Crystal Structure and Chemical Properties of U$_{2}$Al$_{3}$C$_{4}$ and Structure Refinement of Al$_{4}$C$_{3}$, Z. Naturforsch. B 50, 196–200 (1995), doi:10.1515/znb-1995-0206.

Prototype Generator

aflow --proto=A4B3_hR7_166_2c_ac --params=$a,c/a,x_{2},x_{3},x_{4}$

Species:

Running:

Output: