α-Hg (A10) Structure: A_hR1_166_a-002
| Prototype | Hg |
| AFLOW prototype label | A_hR1_166_a-002 |
| Strukturbericht designation | $A10$ |
| ICSD | 174006 |
| Pearson symbol | hR1 |
| Space group number | 166 |
| Space group symbol | $R\overline{3}m$ |
| AFLOW prototype command |
aflow --proto=A_hR1_166_a-002
--params=$a, \allowbreak c/a$ |
- This rhombohedral structure becomes cubic at various values of $c/a$ (or $\alpha$) to wit,
$c/a$ $\alpha$ Cubic Lattice $\sqrt{6}$ $60°$ Face-Centered Cubic $\sqrt{\frac32}$ $90°$ Simple Cubic $\sqrt{\frac38}$ $109.47°$ Body-Centered Cubic
- $\beta$–Po (A_hR1_166_a and $\alpha$–Hg (A_hR1_166_a) have the same AFLOW prototype label. They are generated by the same symmetry operations with different sets of parameters (
--params) specified in their corresponding CIF files. Experimentally, $\beta$–Po ($A_{i}$) has c/a near 1, or $\alpha > 90°$, while $\alpha$–Hg (A10) has c/a near 2, or $\alpha < 90°$. - Hexagonal settings of rhombohedral structures can be obtained with the option
--hex.
\[ \begin{array}{ccc}
\mathbf{a_{1}}&=&\frac{1}{2}a \,\mathbf{\hat{x}}- \frac{\sqrt{3}}{6}a \,\mathbf{\hat{y}}+\frac{1}{3}c \,\mathbf{\hat{z}}\\\mathbf{a_{2}}&=&\frac{1}{\sqrt{3}}a \,\mathbf{\hat{y}}+\frac{1}{3}c \,\mathbf{\hat{z}}\\\mathbf{a_{3}}&=&- \frac{1}{2}a \,\mathbf{\hat{x}}- \frac{\sqrt{3}}{6}a \,\mathbf{\hat{y}}+\frac{1}{3}c \,\mathbf{\hat{z}}
\end{array}\]
Basis vectors
| Lattice coordinates | Cartesian coordinates | Wyckoff position | Atom type | |||
|---|---|---|---|---|---|---|
| $\mathbf{B_{1}}$ | = | $0$ | = | $0$ | (1a) | Hg I |
References
- C. S. Barrett, The structure of mercury at low temperatures, Acta Cryst. 10, 58–60 (1957), doi:10.1107/S0365110X57000134.
Found in
- J. Donohue, The Structures of the Elements (Robert E. Krieger Publishing Company, New York, 1974).
Prototype Generator
aflow --proto=A_hR1_166_a --params=$a,c/a$