Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: A5B2_oP14_49_cehq_ab-001

This structure originally had the label A5B2_oP14_49_dehq_ab. 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/XVUH
or https://aflow.org/p/A5B2_oP14_49_cehq_ab-001
or PDF Version

β-Ta$_{2}$O$_{5}$ Structure: A5B2_oP14_49_cehq_ab-001

Picture of Structure; Click for Big Picture
Prototype O$_{5}$Ta$_{2}$
AFLOW prototype label A5B2_oP14_49_cehq_ab-001
ICSD 95462
Pearson symbol oP14
Space group number 49
Space group symbol $Pccm$
AFLOW prototype command aflow --proto=A5B2_oP14_49_cehq_ab-001
--params=$a, \allowbreak b/a, \allowbreak c/a, \allowbreak x_{6}, \allowbreak y_{6}$

  • (Aleshina, 2002) place this structure in space group $Pccm$ #49, while AFLOW's (and VASP's) default tolerance halves the size of the $c$-axis and places the system in space group $Pmmm$ #47. The reported structure can be recovered using
  • aflow --proto=A5B2_oP14_49_cehq_ab:O:Ta --params=a,b/a,c/a,x$_{6}$,y$_{6}$ --tolerance=0.001 .
  • It is likely that first-principles calculations starting from this point will relax produce a structure equivalent to the smaller $Pmmm$ unit cell.

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

Basis vectors

Lattice coordinates Cartesian coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $0$ = $0$ (2a) Ta I
$\mathbf{B_{2}}$ = $\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}c \,\mathbf{\hat{z}}$ (2a) Ta I
$\mathbf{B_{3}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}b \,\mathbf{\hat{y}}$ (2b) Ta II
$\mathbf{B_{4}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}b \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}$ (2b) Ta II
$\mathbf{B_{5}}$ = $\frac{1}{2} \, \mathbf{a}_{2}$ = $\frac{1}{2}b \,\mathbf{\hat{y}}$ (2c) O I
$\mathbf{B_{6}}$ = $\frac{1}{2} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}b \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}$ (2c) O I
$\mathbf{B_{7}}$ = $\frac{1}{4} \, \mathbf{a}_{3}$ = $\frac{1}{4}c \,\mathbf{\hat{z}}$ (2e) O II
$\mathbf{B_{8}}$ = $\frac{3}{4} \, \mathbf{a}_{3}$ = $\frac{3}{4}c \,\mathbf{\hat{z}}$ (2e) O II
$\mathbf{B_{9}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}+\frac{1}{4} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}b \,\mathbf{\hat{y}}+\frac{1}{4}c \,\mathbf{\hat{z}}$ (2h) O III
$\mathbf{B_{10}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}+\frac{3}{4} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}b \,\mathbf{\hat{y}}+\frac{3}{4}c \,\mathbf{\hat{z}}$ (2h) O III
$\mathbf{B_{11}}$ = $x_{6} \, \mathbf{a}_{1}+y_{6} \, \mathbf{a}_{2}$ = $a x_{6} \,\mathbf{\hat{x}}+b y_{6} \,\mathbf{\hat{y}}$ (4q) O IV
$\mathbf{B_{12}}$ = $- x_{6} \, \mathbf{a}_{1}- y_{6} \, \mathbf{a}_{2}$ = $- a x_{6} \,\mathbf{\hat{x}}- b y_{6} \,\mathbf{\hat{y}}$ (4q) O IV
$\mathbf{B_{13}}$ = $- x_{6} \, \mathbf{a}_{1}+y_{6} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $- a x_{6} \,\mathbf{\hat{x}}+b y_{6} \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}$ (4q) O IV
$\mathbf{B_{14}}$ = $x_{6} \, \mathbf{a}_{1}- y_{6} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $a x_{6} \,\mathbf{\hat{x}}- b y_{6} \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}$ (4q) O IV

References

  • L. A. Aleshina and S. V. Loginova, Rietveld analysis of X-ray diffraction pattern from $\\beta$-Ta$_{2}$O$_{5}$ oxide}, Crystallogr. Rep. 47, 415–419 (2002), doi:10.1134/1.1481927. Translated from Kristallografiya {\bf 47, 460-464 (2002).
  • H. T. Stokes and D. M. Hatch, {\em FINDSYM}: program for identifying the space-group symmetry of a crystal, Appl. Crystallogr. 38, 237–238 (2005), doi:10.1107/S0021889804031528.
  • D. Hicks, C. Oses, E. Gossett, G. Gomez, R. H. Taylor, C. Toher, M. J. Mehl, O. Levy, and S. Curtarolo, AFLOW-SYM: platform for the complete, automatic and self-consistent symmetry analysis of crystals, Acta Crystallogr. Sect. A 74, 184–203 (2018), doi:10.1107/S2053273318003066.
  • A. L. Speck, Single-crystal structure validation with the program PLATON, Appl. Crystallogr. 36, 7–13 (2003), doi:10.1107/S0021889802022112.

Found in

  • P. Villars and K. Cenzual, Pearson's Crystal Data – Crystal Structure Database for Inorganic Compounds (2013). ASM International.

Prototype Generator

aflow --proto=A5B2_oP14_49_cehq_ab --params=$a,b/a,c/a,x_{6},y_{6}$

Species:

Running:

Output: