Encyclopedia of Crystallographic Prototypes

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

Au$_{2}$Nb$_{3}$ Structure: A2B3_tI10_139_e_ae-001

Picture of Structure; Click for Big Picture
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=$a, \allowbreak c/a, \allowbreak z_{2}, \allowbreak z_{3}$

Other compounds with this structure

Os$_{2}$Al$_{3}$,  Ti$_{2}$Cu$_{3}$


  • (Schubert, 1960) listed the lattice constants in kX units. 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.)
  • When $c/a = 5, z_{2} = 1/5$ and $z_{3} = 2/5$, the atoms are on the sites of a body-centered cubic lattice.

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

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

References

  • K. Schubert, T. R. Anantharaman, H. O. K. Ata, H. G. Meissner, M. Pötzschke, W. Rossteutscher, and E. Stolz, Einige strukturelle Ergebnisse an metallischen Phasen (6), Naturwissenschaften 47, 512 (1960), doi:10.1007/BF00641115.
  • J. W. Arblaster, Crystallographic Properties of Platinum, Platinum Metals Rev. 41, 12–21 (1997).
  • 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, Comput. Mater. Sci. 199, 110450 (2021), doi:10.1016/j.commatsci.2021.110450.

Found in


Prototype Generator

aflow --proto=A2B3_tI10_139_e_ae --params=$a,c/a,z_{2},z_{3}$

Species:

Running:

Output: