Generalized Hopf bifurcation in Hilbert space
- 1 January 1979
- journal article
- research article
- Published by Wiley in Mathematical Methods in the Applied Sciences
- Vol. 1 (4), 498-513
- https://doi.org/10.1002/mma.1670010408
Abstract
We consider a family of semilinear evolution equations in Hilbert space of the form equation image with, in general, unbounded operators *A(λ), F(λ·) depending analytically on a real parameter λ. We assume that the origin is a stationary solution, i.e. F(λ,0) = 0, for all λ ε R and that the linearization (with respect to u) at the origin is given by du/dt + A(λ)u = 0. Our essential assumption is the following: A(λ) possesses one pair of simple complex conjugate eigenvalues μ(λ) = Re μ(λ) ± i Im μ(λ) such that Im μ(0) > 0 and equation image for some m ε N or equation image If m = 1 the curves of eigenvalues μ(λ) cross the imaginary axis transversally at ±i Im μ(0). In this case a unique branch of periodic solutions emanates from the origin at λ = 0 which is commonly called Hopf bifurcation. If μ(λ) and the imaginary axis are no longer transversal, i.e. m > 1, we call a bifurcation of periodic solutions, if it occurs, a generalized Hopf bifurcation. It is remarkable that up to m such branches may exist. Our approach gives the number of bifurcating solutions, their direction of bifurcation, and its asymptotic expansion. We regain the results of D. Flockerzi who established them in a completely different way for ordinary differential equations.This publication has 3 references indexed in Scilit:
- Hopf bifurcation at multiple eigenvaluesArchive for Rational Mechanics and Analysis, 1979
- Perturbation theory for linear operatorsPublished by Springer Nature ,1966
- Sur le polygone de NewtonArchiv der Mathematik, 1949