  Based on a simple model for ordering of hexagons on square planar lattice, an
attempt has been made to consider possible structure of C(_{60}) fullerite in
its low temperature phase. It is shown that hexagons, imitating fullerens
oriented along (C_{3}) axes of \emph{sc} lattice, can be ordered into an ideal
structure with four non-equivalent molecules in unit cell. Then the energy
degeneracy for each hexagon rotations by (\pi /3) around its (C_{3}) axis
leaves the translational and orientational order in this structure, but leads
to a random distribution of (\pi /3) rotations and hence to {}``averaged{}''
unit cell with two molecules. However the most relevant structural defects are
not these intrinsic \char`\"{}misorientations\char`\"{} but certain walls
between the domains with different sequencies of the above-mentioned two
(non-ideal) sublattices. Numeric estimates have been made for the anisotropic
inter-molecular potential showing that the anisotropy is noticeably smaller for
molecules in walls than in domains.
