When $c/a=\sqrt{2/3}≈ 0.861$ the coordination number of this system is 10, as the atoms at the points $(0,0,\pm c)$ are at the same distance from the atom at the origin as the atoms at $(\pm a/2,\pm a/2,\pm c/2)$. In protactinium $c/a = 0.823$.
We take our data from (Zachariasen, 1959), but the ICSD entry is from the later work of (Benedict, 1982).
The indium ($A6$) and protactinium ($A_{a}$) structures have the same AFLOW prototype label, A_tI2_139_a. They are generated by the same symmetry operations with different sets of parameters (--params) specified in their corresponding CIF files.
The ICSD lists both structures under the high-pressure Sn(tI2) structure type. We instead follow the Strukturbericht designation and assign structures with $c/a > 1$ to $A6$ while $A_{a}$ has $c/a < 1$.
W. H. Zachariasen, On the crystal structure of protactinium metal, Acta Cryst. 12, 698–700 (1959), doi:10.1107/S0365110X59002043.
U. Benedict, J. C. Spirlet, C. Doufour, I. Birkel, W. B. Holzapfle, and J. R. Petersen, X-ray diffraction study of protactinium metal to 53 GPa, J. Magn. Magn. Mater. 29, 287–290 (1982), doi:10.1016/0304-8853(82)90252-9.
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)