BaZnSb$_{2}$ Structure: AB2C_tI16_139_e_ce_d-003
Prototype
BaSb$_{2}$Zn
AFLOW prototype label
AB2C_tI16_139_e_ce_d-003
ICSD 52694
CCDC 1617425
Pearson symbol
tI16
Space group number
139
Space group symbol
$I4/mmm$
AFLOW prototype command
aflow --proto=AB2C_tI16_139_e_ce_d-003
--params=$a, \allowbreak c/a, \allowbreak z_{3}, \allowbreak z_{4}$
Other compounds with this structure
BaCdBi$_{2}$, BaCdSb$_{2}$, BaMnSb$_{2}$, BaZnBi$_{2}$, SrCdBi$_{2}$, SrZnBi$_{2}$
Many authorities designate SrZnBi$_{2}$ as the prototype for this structure.
\[ \begin{array}{ccc}
\mathbf{a_{1}}&=&- \frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}a \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}\\\mathbf{a_{2}}&=&\frac{1}{2}a \,\mathbf{\hat{x}}- \frac{1}{2}a \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}\\\mathbf{a_{3}}&=&\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}a \,\mathbf{\hat{y}}- \frac{1}{2}c \,\mathbf{\hat{z}}
\end{array}\]
Basis vectors
Lattice
coordinates Cartesian
coordinates Wyckoff position Atom type
$\mathbf{B_{1}}$ = $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{y}}$ (4c) Sb I
$\mathbf{B_{2}}$ = $\frac{1}{2} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ = $\frac{1}{2}a \,\mathbf{\hat{x}}$ (4c) Sb 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) Zn 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) Zn I
$\mathbf{B_{5}}$ = $z_{3} \, \mathbf{a}_{1}+z_{3} \, \mathbf{a}_{2}$ = $c z_{3} \,\mathbf{\hat{z}}$ (4e) Ba I
$\mathbf{B_{6}}$ = $- z_{3} \, \mathbf{a}_{1}- z_{3} \, \mathbf{a}_{2}$ = $- c z_{3} \,\mathbf{\hat{z}}$ (4e) Ba I
$\mathbf{B_{7}}$ = $z_{4} \, \mathbf{a}_{1}+z_{4} \, \mathbf{a}_{2}$ = $c z_{4} \,\mathbf{\hat{z}}$ (4e) Sb II
$\mathbf{B_{8}}$ = $- z_{4} \, \mathbf{a}_{1}- z_{4} \, \mathbf{a}_{2}$ = $- c z_{4} \,\mathbf{\hat{z}}$ (4e) Sb II
References
E. Brechtel, G. Cordier, and H. Schäfer, Neue ternäre erdalkali-übergangselement-pnictide , J. Less-Common Met. 79 , 131–138 (1981), doi:10.1016/0022-5088(81)90057-6 .
Found in
C. Yi, S. Yang, M. Yang, L. Wang, Y. Matsushita, S. Miao, Y. Jiao, J. Cheng, Y. Li, K. Yamaura, Y. Shi, and J. Luo, Large negative magnetoresistance of a nearly Dirac material: Layered antimonide EuMnSb$_{2}$ , Phys. Rev. B 96 , 205103 (2017), doi:10.1103/PhysRevB.96.205103 .
First cited in
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 , Comp. Mat. Sci. 240 , 112988 (2024). (doi=10.1016/j.commatsci.2021.110450 )
Prototype Generator
aflow --proto=AB2C_tI16_139_e_ce_d --params= $a,c/a,z_{3},z_{4}$
VASP Output
QE Output
FHI-AIMS Output
ABINIT Output
WYCCAR Output
CIF Output
ELK Output
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