A fixed point is locally attracting when its multiplier satisfies and repelling when . A multiplier crossing can create or destroy fixed points in a fold bifurcation, or exchange their stability when branches cross, as in a transcritical bifurcation. A multiplier crossing gives a flip, or period-doubling bifurcation, in which a two-cycle can emerge. These are the two multiplier mechanisms; additional symmetry can distinguish special cases at .
For the logistic map, the fixed points are
The second lies in only for . Their multipliers are and . Thus zero attracts for ; the branches meet at and exchange stability, with the nonzero branch attracting for . At , positive orbits decrease to zero since . At , put . Then and its second iterate is
so the fixed point is still weakly attracting at the bifurcation, although linear attraction has disappeared.
The supplied factorization gives the nonfixed two-cycle points for :
They are interchanged by . Using their sum and product in gives
The two-cycle is attracting exactly for
It is born from the fixed point at multiplier for the second iterate, and at its multiplier reaches , giving the next period doubling. The boundary cycles are nonhyperbolic; the strict multiplier test is not a proof of attraction there.
Beyond this threshold the logistic map undergoes further period doublings, with attracting cycles of periods and then chaotic parameter ranges, interspersed with periodic windows. It is not correct to say that every parameter above this threshold is chaotic. At , the substitution gives , illustrating its chaotic doubling-map behavior.

Articles by others on the same topic (0)

There are currently no matching articles.