This criterion holds even for reducible nonnegative matrices. If a fixed point exists, for gives on its support. Some therefore satisfies , forcing the spectral radius above one by the Perron–Frobenius theorem. Conversely take , , with and . For sufficiently small , . Thus is a subsolution; monotone iteration under gives a positive fixed point below . Strictness of excludes survival at the critical value for this Poisson offspring law.
In the nested partial unary operation category, suppose the lower-operation diagram has a split coequalizer with , and . The section takes eligible fixed points to eligible fixed points, so the displayed next operation is defined on exactly the required domain. For eligible , the equations give
Thus preserves the next operation. Every factored morphism preserves it by evaluating at , giving creation of the specified coequalizer. Together with reflection of isomorphisms, the Beck monadicity theorem proves one-step monadicity.
Here is the low-density per-generation multiplication factor and sets the inverse crowding scale. The positive fixed point is when ; its derivative lies strictly between minus one and one, so it is locally asymptotically stable. The map reaches its maximum at and decreases thereafter. Stability follows from the derivative, not from assuming that every overcompensating population map undergoes period doubling.
A self-map of a nonempty compact metric space satisfying the displayed strict distance inequality has exactly one fixed point, although a uniform contraction constant need not exist. The inequality makes Lipschitz continuous with constant at most one, so is continuous and attains a minimum at . If , then , a contradiction. Two different fixed points contradict the same distance inequality.
At a strong resonance of a planar map the Floquet multiplier of a fixed point is a root of unity of low order. The usual nonresonant Neimark–Sacker bifurcation requires for . At a 1:3 resonance a quadratic term cannot be removed from the normal form; at a 1:4 resonance a cubic term remains. Consequently one cannot infer a quasiperiodic invariant curve from the unit-modulus crossing alone.
Surjectivity of a continuous bounded-displacement map Created 2026-10-05 Updated 2026-10-14
If a continuous map has , then it is onto. For a target , choose , , and map the unit ball to itself by . A fixed point gives .
A fixed point of the th iteration of a map of a subshift of finite type is determined uniquely by its length- block with a permitted closing transition. Summing the counts of length- closed walks over their starting symbols gives the displayed trace. This counts points whose least period divides . If counts points of least period exactly , then , and Möbius inversion gives . The number of distinct least-period- periodic orbits is .
Wilson-Fisher fixed point Created 2026-09-24 Updated 2026-10-14
Below four dimensions, the scalar quartic theory has an interacting Wilson-Fisher fixed point that controls the Ising universality class.
This is a particular fixed point of the renormalization group, governing the long-distance behavior of a critical phenomenon.
Winning-position attractor in an infinite game Created 2026-10-06 Updated 2026-10-14
Start with positions whose entire extension cylinder set lies in the winning open set. At each successor stage add I-positions with some successor already present and II-positions with every successor already present; take unions at limit ordinals. The stable set is the least fixed point of this order-preserving operation. The first entry ordinal supplies a strictly decreasing rank until the winning prefix is reached.