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)
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)
This rhombohedral structure becomes cubic at various values of $c/a$ (or $\alpha$) to wit, \[ \begin{array}{ccc}
\mbox{$\textbf{$c/a$}$} & \mathbf{\alpha} & \mbox{$\textbf{Cubic Lattice}$} \\
\sqrt{6} & 60^{o} & \href{A_cF4_225_a.html}{\mbox{Face-Centered Cubic}} \\
\sqrt{\frac{3}{2}} & 90^{o} & \href{A_cP1_221_a.html}{\mbox{Simple Cubic}} \\
\sqrt{\frac{3}{8}} & 109.47^{o} & \href{A_cI2_229_a.html}{\mbox{Body-Centered Cubic}} \\
\end{array}
\]Note that $\beta$–Po (A_hR1_166_a, $\beta$–Po) and $\alpha$–Hg (A_hR1_166_a, $\alpha$–Hg) 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 (Ai) has c/a near 1, or $\alpha$ > 90$^{o}$, while $\alpha$–Hg (A10) has c/a near 2, or $\alpha$ < 90$^{o}$. Hexagonal settings of this structure can be obtained with the option ––hex.