A genuine two-cycle must have the form with . Hence . Subtracting gives
Let and . Using in either original equation gives . The cubic swap-map two-cycle factorization exhibits two cases, so cancellation of would lose an actual branch.
If , then and . Thus the source's quadratic holds for this family, with
There are two reflected genuine cycles for , coalescing with the fixed points at . For their two-step Jacobian matrix, and . The unit-disk necessary inequality fails, since it is . Therefore these quadratic-family cycles are unstable for every . For these unstable asymmetric cycles of a cubic swap map, their periodic-orbit multipliers are real: one exceeds , while the other crosses at . They are saddles before that secondary threshold and repelling beyond it. Their presence on the stable side of the fixed-point flip identifies the unstable branch of a subcritical flip.
If , then and the preceding quadratic identity gives . Hence there is also the exact cycle
This antipodal cycle of a cubic swap map does not satisfy the printed condition: its product is . Along it the one-step Jacobian matrix is the same matrix at both points, so the cycle periodic-orbit multipliers are the squares of the roots of . The Jury stability criterion conditions give
At its periodic-orbit multipliers are on the unit circle and linearization is inconclusive. Its real-to-complex transition occurs at . Thus the printed assertion about all period-two components is incomplete: it describes only , whereas the omitted antipodal cycle supplies the actual stable period-two interval.