AFLOW Prototype: A2BCD2_tI12_139_e_a_b_d-001
If you are using this page, please cite:
H. Eckert, S. Divilov, M. J. Mehl, D. Hicks, A. C. Zettel, M. Esters. X. Campilongo and S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 4. Submitted to Computational Materials Science.
Links to this page
https://aflow.org/p/4LX6
or
https://aflow.org/p/A2BCD2_tI12_139_e_a_b_d-001
or
PDF Version
Prototype | B$_{2}$CLuNi$_{2}$ |
AFLOW prototype label | A2BCD2_tI12_139_e_a_b_d-001 |
ICSD | 75609 |
Pearson symbol | tI12 |
Space group number | 139 |
Space group symbol | $I4/mmm$ |
AFLOW prototype command |
aflow --proto=A2BCD2_tI12_139_e_a_b_d-001
--params=$a, \allowbreak c/a, \allowbreak z_{4}$ |
GdN$_{2}$B$_{2}$C, LaIr$_{2}$B$_{2}$C, LaN$_{2}$B$_{2}$C, LaPt$_{2}$B$_{2}$C, LaRh$_{2}$B$_{2}$C
Basis vectors
Lattice coordinates | Cartesian coordinates | Wyckoff position | Atom type | |||
---|---|---|---|---|---|---|
$\mathbf{B_{1}}$ | = | $0$ | = | $0$ | (2a) | C I |
$\mathbf{B_{2}}$ | = | $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}$ | = | $\frac{1}{2}c \,\mathbf{\hat{z}}$ | (2b) | Lu I |
$\mathbf{B_{3}}$ | = | $\frac{3}{4} \, \mathbf{a}_{1}+\frac{1}{4} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{y}}+\frac{1}{4}c \,\mathbf{\hat{z}}$ | (4d) | Nd I |
$\mathbf{B_{4}}$ | = | $\frac{1}{4} \, \mathbf{a}_{1}+\frac{3}{4} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{4}c \,\mathbf{\hat{z}}$ | (4d) | Nd I |
$\mathbf{B_{5}}$ | = | $z_{4} \, \mathbf{a}_{1}+z_{4} \, \mathbf{a}_{2}$ | = | $c z_{4} \,\mathbf{\hat{z}}$ | (4e) | B I |
$\mathbf{B_{6}}$ | = | $- z_{4} \, \mathbf{a}_{1}- z_{4} \, \mathbf{a}_{2}$ | = | $- c z_{4} \,\mathbf{\hat{z}}$ | (4e) | B I |