AFLOW Prototype: A6B2C_cF36_225_e_c_a-001
This structure originally had the label A6B2C_cF36_225_e_c_a. 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/L6LF
or
https://aflow.org/p/A6B2C_cF36_225_e_c_a-001
or
PDF Version
Prototype | Cl$_{6}$K$_{2}$Pt |
AFLOW prototype label | A6B2C_cF36_225_e_c_a-001 |
Strukturbericht designation | $J1_{1}$ |
ICSD | 31114 |
Pearson symbol | cF36 |
Space group number | 225 |
Space group symbol | $Fm\overline{3}m$ |
AFLOW prototype command |
aflow --proto=A6B2C_cF36_225_e_c_a-001
--params=$a, \allowbreak x_{3}$ |
Ba$_{2}$RuH$_{6}$, Ca$_{2}$FeH$_{6}$, Ca$_{2}$OsH$_{6}$, Ca$_{2}$RuH$_{6}$, Cs$_{2}$CoF$_{6}$, Cs$_{2}$CsF$_{6}$, Cs$_{2}$GeCl$_{6}$, Cs$_{2}$GeF$_{6}$, Cs$_{2}$MnCl$_{6}$, Cs$_{2}$NbI$_{6}$, Cs$_{2}$PbCl$_{6}$, Cs$_{2}$PdBr$_{6}$, Cs$_{2}$PtCl$_{6}$, Cs$_{2}$SnBr$_{6}$, Cs$_{2}$SnCl$_{6}$, Cs$_{2}$SnI$_{6}$, Cs$_{2}$TeCl$_{6}$, Cs$_{2}$TiCl$_{6}$, Cs$_{2}$TlCl$_{6}$, Cs$_{2}$ZrCl$_{6}$, Gd$_{2}$MnGa$_{6}$, K$_{2}$MnCl$_{6}$, K$_{2}$OsBr$_{2}$, K$_{2}$OsCl$_{6}$, K$_{2}$PtCl$_{6}$, K$_{2}$PtCl$_{6}$, K$_{2}$ReCl$_{6}$, K$_{2}$SnBr$_{6}$, K$_{2}$SnCl$_{6}$, K$_{2}$SnI$_{6}$, K$_{2}$TeBr$_{6}$, Mg$_{2}$FeH$_{6}$, Mg$_{2}$OsH$_{6}$, Mg$_{2}$RuH$_{6}$, Rb$_{2}$MnCl$_{6}$, Rb$_{2}$PbCl$_{6}$, Rb$_{2}$PdCl$_{6}$, Rb$_{2}$PtCl$_{6}$, Rb$_{2}$SeCl$_{6}$, Rb$_{2}$SnBr$_{6}$, Rb$_{2}$SnCl$_{6}$, Rb$_{2}$SnI$_{6}$, Rb$_{2}$TaBr$_{6}$, Rb$_{2}$TeCl$_{6}$, Rb$_{2}$ZrCl$_{6}$, Sr$_{2}$FeH$_{6}$, Sr$_{2}$OsH$_{6}$, Sr$_{2}$RuH$_{6}$, Tl$_{2}$SnCl$_{6}$, (NH$_{4}$)$_{2}$PbCl$_{6}$, (NH$_{4}$)$_{2}$PtCl$_{6}$, (NH$_{4}$)$_{2}$SbCl$_{6}$, (NH$_{4}$)$_{2}$SiF$_{6}$, (NH$_{4}$)$_{2}$SnCl$_{6}$, Br$_{2}$Ni(NH$_{3}$)$_{6}$, Cl$_{2}$Co(NH$_{3}$)$_{6}$, Cs$_{2}$Ni(NH$_{3}$)$_{6}$, I$_{2}$Co(NH$_{3}$)$_{6}$, I$_{2}$Ni(NH$_{3}$)$_{6}$
Basis vectors
Lattice coordinates | Cartesian coordinates | Wyckoff position | Atom type | |||
---|---|---|---|---|---|---|
$\mathbf{B_{1}}$ | = | $0$ | = | $0$ | (4a) | Pt I |
$\mathbf{B_{2}}$ | = | $\frac{1}{4} \, \mathbf{a}_{1}+\frac{1}{4} \, \mathbf{a}_{2}+\frac{1}{4} \, \mathbf{a}_{3}$ | = | $\frac{1}{4}a \,\mathbf{\hat{x}}+\frac{1}{4}a \,\mathbf{\hat{y}}+\frac{1}{4}a \,\mathbf{\hat{z}}$ | (8c) | K I |
$\mathbf{B_{3}}$ | = | $\frac{3}{4} \, \mathbf{a}_{1}+\frac{3}{4} \, \mathbf{a}_{2}+\frac{3}{4} \, \mathbf{a}_{3}$ | = | $\frac{3}{4}a \,\mathbf{\hat{x}}+\frac{3}{4}a \,\mathbf{\hat{y}}+\frac{3}{4}a \,\mathbf{\hat{z}}$ | (8c) | K I |
$\mathbf{B_{4}}$ | = | $- x_{3} \, \mathbf{a}_{1}+x_{3} \, \mathbf{a}_{2}+x_{3} \, \mathbf{a}_{3}$ | = | $a x_{3} \,\mathbf{\hat{x}}$ | (24e) | Cl I |
$\mathbf{B_{5}}$ | = | $x_{3} \, \mathbf{a}_{1}- x_{3} \, \mathbf{a}_{2}- x_{3} \, \mathbf{a}_{3}$ | = | $- a x_{3} \,\mathbf{\hat{x}}$ | (24e) | Cl I |
$\mathbf{B_{6}}$ | = | $x_{3} \, \mathbf{a}_{1}- x_{3} \, \mathbf{a}_{2}+x_{3} \, \mathbf{a}_{3}$ | = | $a x_{3} \,\mathbf{\hat{y}}$ | (24e) | Cl I |
$\mathbf{B_{7}}$ | = | $- x_{3} \, \mathbf{a}_{1}+x_{3} \, \mathbf{a}_{2}- x_{3} \, \mathbf{a}_{3}$ | = | $- a x_{3} \,\mathbf{\hat{y}}$ | (24e) | Cl I |
$\mathbf{B_{8}}$ | = | $x_{3} \, \mathbf{a}_{1}+x_{3} \, \mathbf{a}_{2}- x_{3} \, \mathbf{a}_{3}$ | = | $a x_{3} \,\mathbf{\hat{z}}$ | (24e) | Cl I |
$\mathbf{B_{9}}$ | = | $- x_{3} \, \mathbf{a}_{1}- x_{3} \, \mathbf{a}_{2}+x_{3} \, \mathbf{a}_{3}$ | = | $- a x_{3} \,\mathbf{\hat{z}}$ | (24e) | Cl I |