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 $\alpha$)
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.
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)