AFLOW Prototype: A2B3_tI10_139_e_ae-001
This structure originally had the label A2B3_tI10_139_e_ae. Calls to that address will be redirected here.
If you are using this page, please cite:
D. Hicks, M.J. Mehl, M. Esters, C. Oses, O. Levy, G.L.W. Hart, C. Toher, and S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 3, Comp. Mat. Sci. 199, 110450 (2021). (doi=10.1016/j.commatsci.2021.110450)
Links to this page
https://aflow.org/p/5STC
or
https://aflow.org/p/A2B3_tI10_139_e_ae-001
or
PDF Version
Prototype | Au$_{2}$Nb$_{3}$ |
AFLOW prototype label | A2B3_tI10_139_e_ae-001 |
ICSD | 58559 |
Pearson symbol | tI10 |
Space group number | 139 |
Space group symbol | $I4/mmm$ |
AFLOW prototype command |
aflow --proto=A2B3_tI10_139_e_ae-001
--params=$a, \allowbreak c/a, \allowbreak z_{2}, \allowbreak z_{3}$ |
Os$_{2}$Al$_{3}$, Ti$_{2}$Cu$_{3}$
kXunits. We used the conversion factor 1.00207789 to convert their units into Ångstroms (Arblaster, 1997). (We had previously (Hicks, 2021) divided instead of multiplied. This has been corrected.)
Basis vectors
Lattice coordinates | Cartesian coordinates | Wyckoff position | Atom type | |||
---|---|---|---|---|---|---|
$\mathbf{B_{1}}$ | = | $0$ | = | $0$ | (2a) | Nb I |
$\mathbf{B_{2}}$ | = | $z_{2} \, \mathbf{a}_{1}+z_{2} \, \mathbf{a}_{2}$ | = | $c z_{2} \,\mathbf{\hat{z}}$ | (4e) | Au I |
$\mathbf{B_{3}}$ | = | $- z_{2} \, \mathbf{a}_{1}- z_{2} \, \mathbf{a}_{2}$ | = | $- c z_{2} \,\mathbf{\hat{z}}$ | (4e) | Au I |
$\mathbf{B_{4}}$ | = | $z_{3} \, \mathbf{a}_{1}+z_{3} \, \mathbf{a}_{2}$ | = | $c z_{3} \,\mathbf{\hat{z}}$ | (4e) | Nb II |
$\mathbf{B_{5}}$ | = | $- z_{3} \, \mathbf{a}_{1}- z_{3} \, \mathbf{a}_{2}$ | = | $- c z_{3} \,\mathbf{\hat{z}}$ | (4e) | Nb II |