Encyclopedia of Crystallographic Prototypes

AFLOW Prototype: A_hR1_166_a-001

This structure previously used the label(s) A_hR1_166_a.beta-Po. Calls to these addresses will be redirected here.

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https://aflow.org/p/RUSN
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β-Po ($A_i$) Structure: A_hR1_166_a-001

Picture of Structure; Click for Big Picture
Prototype Po
AFLOW prototype label A_hR1_166_a-001
Strukturbericht designation $A_{i}$
ICSD 649161
CCDC 1763583
Pearson symbol hR1
Space group number 166
Space group symbol $R\overline{3}m$
AFLOW prototype command aflow --proto=A_hR1_166_a-001
--params=$a, \allowbreak c/a$

  • Originally, Po was assigned Strukturbericht designation $A19$, which is now considered to be incorrect. (Donohue, 1982, 390).
  • Solid polonium actually exists in two phases: cubic $\alpha$–Po ($A_{h}$) is the ground state and rhombohedral $\beta$–Po ($A_{l}$) (this structure) (Donohue, 1974). There is a large amount of hysteresis observed in the transition, which occurs at 54$^\circ$C for $\alpha \rightarrow \beta$ and 18$^\circ$ for $\beta \rightarrow \alpha$.
  • This rhombohedral structure becomes cubic at various values of c/a (or $\alpha$)

    $c/a$ $\alpha$ Cubic Lattice
    $\sqrt{7}$ $60°$ Face-Centered Cubic
    $\sqrt{\frac32}$ $90°$ Simple Cubic
    $\sqrt{\frac38}$ $109.47°$ Body-Centered Cubic

  • Note that $\beta$–Po and $\alpha$–Hg have the same AFLOW prototype label, A_hR1_166_a. 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) Po I

References

  • W. H. Beamer and C. L. Maxwell, Physical Properties of Polonium. II. X-Ray Studies and Crystal Structure, J. Chem. Phys. 17, 1293–1298 (1949), doi:10.1063/1.1747155.

Found in

  • J. Donohue, The Structures of the Elements (Robert E. Krieger Publishing Company, New York, 1974).

First cited in

  • M. J. Mehl, D. Hicks, C. Toher, O. Levy, R. M. Hanson, G. L. W. Hart, and S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 1, Comp. Mat. Sci. 136, S1-S828 (2017). (doi=10.1016/j.commatsci.2017.01.017)

Geometry files


Prototype Generator

aflow --proto=A_hR1_166_a --params=$a,c/a$

Species:

Running:

Output: