Let be rotation through about , and let be rotation through about . These generate the order-six dihedral group with relations
namely . We specify its order explicitly because dihedral notation has two conventions. It is a proper finite subgroup of the full axial rotation group.
To see that it is sufficient, write a general matrix in blocks . Commutation with forces , since a nontrivial planar -degree rotation fixes no nonzero planar vector. Its planar part is , with nonzero sine, so must commute with and has the form . Commutation with again kills . Hence this six-element subgroup has precisely the required invariant tensors.
It is also smallest by order. Groups of orders are cyclic: a nonidentity element has order dividing the prime group order by Lagrange theorem. For a cyclic rotation subgroup, the nonzero antisymmetric tensor representing cross product with its rotation-axis direction is invariant, so it cannot force the symmetric form above. The trivial subgroup plainly imposes no constraint. A group of order four is either cyclic or has three nonidentity elements of order two; in the latter case they commute, since and also equals . Commuting distinct half-turns in three dimensions have perpendicular axes: conjugation by one half-turn must preserve the other's axis, and a distinct preserved axis lies in its perpendicular plane. In the specified axial group, their three axes are consequently and two perpendicular horizontal directions. In coordinates along them every diagonal matrix is invariant, including one with unequal horizontal entries. Such a group again does not force the required form.
Thus the smallest subgroup has six elements, generated by the axial -degree rotation and one horizontal half-turn. It is the smallest axial rotation group forcing second-rank transverse isotropy; conjugating the horizontal axis gives equally valid choices.