English

Renormalization of three dimensional H\'enon map I : Reduction of ambient space

Dynamical Systems 2014-08-20 v1

Abstract

Three dimensional analytic H\'enon-like map F(x,y,z)=(f(x)ϵ(x,y,z),x,δ(x,y,z)) F(x,y,z) = (f(x) - \epsilon(x,y,z),\, x,\, \delta(x,y,z)) and its {\em period doubling} renormalization is defined. If F F is infinitely renormalizable map, Jacobian determinant of nth n^{th} renormalized map, RnF R^nF has asymptotically universal expression JacRnF=bF2na(x)(1+O(ρn)) Jac R^nF = b_F^{2^n}a(x)(1 + O(\rho^n)) where bF b_F is the average Jacobian of F F . The toy model map, Fmod F_{mod} is defined as the map satisfying zϵ0 \partial_z \epsilon \equiv 0 . The set of toy model map is invariant under renormalizaton. Moreover, if zδyϵ \| \partial_z \delta \| \ll \| \partial_y \epsilon \| , then there exists the continuous invariant plane field over OF \mathcal O_F with dominated splitting. Under this condition, three dimensional H\'enon-like map %with the dominated splitting is dynamically decomposed into two dimensional map with contraction along the strong stable direction. Any invariant line field on this plane filed over OFmod \mathcal O_{F_{mod}} cannot be continuous.

Keywords

Cite

@article{arxiv.1408.4289,
  title  = {Renormalization of three dimensional H\'enon map I : Reduction of ambient space},
  author = {Young Woo Nam},
  journal= {arXiv preprint arXiv:1408.4289},
  year   = {2014}
}