AFLOW Prototype: AB8C2_tP11_123_a_ehi_g-003
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| Prototype | CoGa$_{8}$Ho$_{2}$ |
| AFLOW prototype label | AB8C2_tP11_123_a_ehi_g-003 |
| ICSD | 198243 |
| CCDC | 1925146 |
| Pearson symbol | tP11 |
| Space group number | 123 |
| Space group symbol | $P4/mmm$ |
| AFLOW prototype command |
aflow --proto=AB8C2_tP11_123_a_ehi_g-003
--params=$a, \allowbreak c/a, \allowbreak z_{3}, \allowbreak z_{4}, \allowbreak z_{5}$ |
Ce$_{2}$CoIn$_{8}$, Ce$_{2}$PdIn$_{8}$, Ce$_{2}$PtIn$_{8}$, Ce$_{2}$RhIn$_{8}$, Dy$_{2}$CoGa$_{8}$, Dy$_{2}$CoIn$_{8}$, Dy$_{2}$FeGa$_{8}$, Er$_{2}$CoGa$_{8}$, Er$_{2}$CoIn$_{8}$, Er$_{2}$FeGa$_{8}$, Gd$_{2}$CoGa$_{8}$, Gd$_{2}$CoIn$_{8}$, Ho$_{2}$CoGa$_{8}$, Ho$_{2}$CoIn$_{8}$, Ho$_{2}$DyGa$_{8}$, Ho$_{2}$ErGa$_{8}$, Ho$_{2}$FeGa$_{8}$, Ho$_{2}$GdGa$_{8}$, Ho$_{2}$LuGa$_{8}$, Ho$_{2}$RhIn$_{8}$, Ho$_{2}$SmGa$_{8}$, Ho$_{2}$TbGa$_{8}$, Ho$_{2}$TmGa$_{8}$, Ho$_{2}$YGa$_{8}$, In$_{2}$AsPt$_{8}$, Nd$_{2}$CoIn$_{8}$, Nd$_{2}$CoPd$_{8}$, Ce$_{2}$CoIn$_{8}$, Ce$_{2}$PdIn$_{8}$, Ce$_{2}$PtIn$_{8}$, Dy$_{2}$CoGa$_{8}$, Dy$_{2}$CoIn$_{8}$, Dy$_{2}$FeGa$_{8}$, Er$_{2}$CoGa$_{8}$, Er$_{2}$CoIn$_{8}$, Er$_{2}$FeGa$_{8}$, Gd$_{2}$CoGa$_{8}$, Gd$_{2}$CoIn$_{8}$, Ho$_{2}$CoGa$_{8}$, Ho$_{2}$CoIn$_{8}$, Ho$_{2}$FeGa$_{8}$, Ho$_{2}$RhIn$_{8}$, In$_{2}$AsPt$_{8}$, In$_{2}$SePd$_{8}$, Lu$_{2}$CoGa$_{8}$, Lu$_{2}$FeGa$_{8}$, Nd$_{2}$CoIn$_{8}$, Nd$_{2}$PdIn$_{8}$, Pr$_{2}$CoIn$_{8}$, Pr$_{2}$PdIn$_{8}$, Sm$_{2}$CoGa$_{8}$, Sm$_{2}$CoIn$_{8}$, Sm$_{2}$PdIn$_{8}$, Tb$_{2}$CoGa$_{8}$, Tb$_{2}$FeGa$_{8}$, Tm$_{2}$CoGa$_{8}$, Tm$_{2}$CoIn$_{8}$, Tm$_{2}$FeGa$_{8}$, U$_{2}$RuGa$_{8}$, U$_{2}$RhIn$_{8}$, Y$_{2}$CoGa$_{8}$, Y$_{2}$CoIn$_{8}$, Yb$_{2}$IrIn$_{8}$, Zn$_{2}$SePd$_{8}$
Basis vectors
| Lattice coordinates | Cartesian coordinates | Wyckoff position | Atom type | |||
|---|---|---|---|---|---|---|
| $\mathbf{B_{1}}$ | = | $0$ | = | $0$ | (1a) | Co I |
| $\mathbf{B_{2}}$ | = | $\frac{1}{2} \, \mathbf{a}_{2}+\frac{1}{2} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{y}}+\frac{1}{2}c \,\mathbf{\hat{z}}$ | (2e) | Ga I |
| $\mathbf{B_{3}}$ | = | $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}c \,\mathbf{\hat{z}}$ | (2e) | Ga I |
| $\mathbf{B_{4}}$ | = | $z_{3} \, \mathbf{a}_{3}$ | = | $c z_{3} \,\mathbf{\hat{z}}$ | (2g) | Ho I |
| $\mathbf{B_{5}}$ | = | $- z_{3} \, \mathbf{a}_{3}$ | = | $- c z_{3} \,\mathbf{\hat{z}}$ | (2g) | Ho I |
| $\mathbf{B_{6}}$ | = | $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}+z_{4} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}a \,\mathbf{\hat{y}}+c z_{4} \,\mathbf{\hat{z}}$ | (2h) | Ga II |
| $\mathbf{B_{7}}$ | = | $\frac{1}{2} \, \mathbf{a}_{1}+\frac{1}{2} \, \mathbf{a}_{2}- z_{4} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{x}}+\frac{1}{2}a \,\mathbf{\hat{y}}- c z_{4} \,\mathbf{\hat{z}}$ | (2h) | Ga II |
| $\mathbf{B_{8}}$ | = | $\frac{1}{2} \, \mathbf{a}_{2}+z_{5} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{y}}+c z_{5} \,\mathbf{\hat{z}}$ | (4i) | Ga III |
| $\mathbf{B_{9}}$ | = | $\frac{1}{2} \, \mathbf{a}_{1}+z_{5} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{x}}+c z_{5} \,\mathbf{\hat{z}}$ | (4i) | Ga III |
| $\mathbf{B_{10}}$ | = | $\frac{1}{2} \, \mathbf{a}_{2}- z_{5} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{y}}- c z_{5} \,\mathbf{\hat{z}}$ | (4i) | Ga III |
| $\mathbf{B_{11}}$ | = | $\frac{1}{2} \, \mathbf{a}_{1}- z_{5} \, \mathbf{a}_{3}$ | = | $\frac{1}{2}a \,\mathbf{\hat{x}}- c z_{5} \,\mathbf{\hat{z}}$ | (4i) | Ga III |