The map normal forms at multiplier are given in the numbered subparts below. For the multiplier problem, the second iterate instead exposes the emerging period-two cycle.
For the multiplier problem, write . To the required weighted order, with , the shifted map is , where . Composing it with itself cancels the quadratic term. The cubic contribution is , while the linear correction is . Consequently the quadratic-cubic flip criticality calculation gives
Thus the second iterate has normal form , up to terms of weighted order at least four. This is the asymptotic interpretation of the stated remainder under ; a uniformly valid local expansion about the exact fixed point also retains mixed parameter remainders.
Assuming crosses zero transversely and , the small nonzero fixed points of the second iterate satisfy . They form a period-two orbit. For they exist on the side , where the original fixed point has become unstable, and the second-iterate multiplier is , so the cycle is stable. The period-doubling bifurcation is therefore supercritical precisely when . Equality is a degenerate case requiring higher-order terms.
For , . The local attracting nonzero segments have or , again subject to ; the segment between the saddle-node and zero repels. The crossings at and one are saddle-node and transcritical. The quadratic-cubic flip criticality at the origin requires additional information: writing gives
It is supercritical if and subcritical if , with a degenerate flip if . The sign assumptions in case (iii) do not determine this criticality. The original “no further bifurcations in the region sketched” qualification is local; it does not remove this possible degeneracy or the additional crossings farther along fixed branches.