A C^1-generic dichotomy for diffeomorphisms: Weak forms of hyperbolicity or infinitely many sinks or sources
By C. Bonatti, Lorenzo J. Díaz, E. Pujals. 2003
330 citations recorded by the source corpus.
Subfields: Geometry and Topology, Mathematical Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/ab64c608a9c079078f0f91091613e5fd2006280a
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Geometry and Topology
- S. Crovisier
- C. Bonatti
- Amie Wilkinson
- A. Tahzibi
- Tom A. Fisher
- Vanderlei Horita
- Nicolas Gourmelon
- Jérôme Buzzi
In Mathematical Physics
- S. Crovisier
- C. Bonatti
- A. Tahzibi
- Nicolas Gourmelon
- Amie Wilkinson
- Tom A. Fisher
- Marcelo Viana
- Vanderlei Horita
In Statistical and Nonlinear Physics
- S. Crovisier
- C. Bonatti
- Nicolas Gourmelon
- A. Tahzibi
- Tom A. Fisher
- Amie Wilkinson
- Vanderlei Horita
- Mart'in Sambarino
Citations in the corpus
- Symbolic extensions for partially hyperbolic diffeomorphisms (2009, neutral): “For a measurable partition ξ and n ∈ N we define the joint partition of ξ with respect to f for n to be the partition (1) ξfn = ξ ∨ f −1(ξ) ∨ · · · ∨ f−n+1(ξ).”
- Stably ergodic diffeomorphisms which are not partially hyperbolic (2002, neutral): “Now suppose gl C U does not admit dominated splitting; by the results in [ 3 ] one can perturb gl to get g2 E U with a sink.”
- Some characterizations of domination (2008, neutral): “D S] 3 1 A ug 2 00 8”
- Maximal entropy measures for certain partially hyperbolic, derived from Anosov systems (2011, background): “Background We now review a few facts on entropy, hyperbolicity, and partial hyperbolicity.”
- Partial hyperbolicity far from homoclinic bifurcations (2008, background): “The class contains periodic orbits whose Lyapunov exponent along Ec 1 is arbitrarily close to 0 and by domination, one deduces that the Lyapunov exponent along Ec 2 for these orbits is larger than a > 0. The same property holds for Ec2: the class contains some periodic orbits whose Lyapunov exponent”