Both and are real symmetric and couple only neighboring sites whose diagonal entries in have opposite signs. For an entry of or , symmetry gives . Every nonzero entry joins signs and , while the diagonal entries vanish. Hence .
The condition is preserved by real linear combinations and commutators, so the entire Dynamical Lie algebra satisfies it. For the physical generator , differentiation gives , and therefore . This is an orthogonal dynamical symmetry in quantum control: a preserved symmetric bilinear form. It need not give eigenspaces of a commuting operator; indeed does not commute with or .
Set . Then , so the transformed generators satisfy as well as . They are consequently real antisymmetric, lying in . The original generators already supply the independent directions and , and their commutator is . These three independent directions exhaust the three-dimensional algebra. Thus
Here denotes a matrix unit. The reachable connected group is a unitary conjugate of , a proper subgroup of , so there is no unitary operator controllability.
Pure-state control also fails. For every reachable state , the quantity is invariant, and its absolute value is unchanged even by an overall state phase. The normalized states and have respectively and , so no allowed control connects their rays. Therefore for this reduced three-level system, despite the absence of a simple excitation-sector obstruction within the sector.