Question (A. Katok): In low dimensions, is every conservative dynamical system with h_\top = 0 a limit of integrable systems?
Low dimensions = 2 dims for maps and 3 dims for flows;
Conservative = area/volume preserving;
Limit = to be defined;
integrable system = a disk map is integrable if exists a function f \colon D \to \R not constant on any open set, \phi^*f = f.
h_\top \in [0, \infty] describes the complexity of the system.
Definition: (h_\top = 0) A pseudorotation is an area preserving disk map
such that \phi(0) = 0 and without any other periodic points.
Franks: a.e. point z \in D \setminus \{ 0 \} has a well defined rotation number about 0. The lack of other periodic points is eqvt (?) to saying these are the same and equal to an irrational number \alpha.
Theorem (Anosov-Katok '70s) There exist ergodic pseudorotations.
In particular a.e. z \in D has a dense orbit.
In particular a.e. z \in D has a dense orbit.
Theorem
Let \phi be a pseudorotation with irrational
rotation number \alpha. There exists a sequence of smooth
\phi_n (fixing 0) which converge to \phi in C^0, and such that
for all n exists diffeo g_n (fixing 0) and p_n/q_n \to \alpha
s.t. \phi_n = g_n^{-1} \circ R_{2\pi p_n/q_n} \circ g_n.
Two questions: can \phi_n be made symplectic? can we obtain higher regularity of convergence?
Remark: if we consider such a sequence of homeo
\phi_n and p_n/q_n \to \alpha, and these C^0-converge to an area preserving homeo \phi, then \phi is a pseudorotation.
Also remark: this is more-or-less how Anosov-Katok construct their examples.
Pseudoholo curves for disk maps
Assume \phi area preserving diffeo. Suspend this to a ``Hamiltonian'' mapping torus. Obtain symplectization \R \times S^1 \times D^2.
The boundary, \R \times S^1 \times \bdy D^2 is filled by two-tori, called L_a = \{ a \} \times S^1 \times \bdy D^2. Totally real.
If \phi non-degenerate then exists a FEF. Some remarks about removal of the condition that the map be a rotation at the boundary, also about existence of many foliations, also existence of FEF with certain prescribed orbits as binding.
Claim: projected map has smooth extension to the boundary!?!?
Approximating pseudorotations
Suppose \phi \in \Diff^\infty( D, \omega_0) is an area preserving disk map.
Take a mapping torus. Lift to universal cover.
Identify each trajectory with a holomorphic curve. Call this a vertical plane. Obtain the vertical foliation.
The claim is that given a vertical (?) foliation, we can construct a map.
Strategy: if \phi is a pseudorotation, find a sequence of foliations so that the d\lambda area is going to 0. Specifically, we have a sequence of foliations so d\lambda is the fractional part of n \alpha, where \alpha is the rot number of \phi. Take a subsequence n_j so this goes to 0.
Each foliation induces a map \phi_{n_j}. The claim is that this converges to \phi since the foliations converge to a vertical foliation.
Furthermore, by the construction, \phi_{n_j}^{(n_j)} = \id.
Note that we used | Per(\phi)| = 1 to know the energies, and also to obtain that each \mathcal F_n is invariant under deck transformations.
somehow, this periodicity tells one that it is ocnjugate to a rational rotation.
Open Question: (Fayad-Katok) Does there exist a strong-mixing area preserving disk map?
Known: suppose that \phi is an irrational pseudorotation. There is some contrast between Diophantine vs Liouville.
Herman showed that Diophantine implies \phi is not strong mixing.
Fayad-Sapryking 2005, Anosov-Katok : any more Liouville than Herman has weak mixing examples.
Barney seems to show that \alpha being sufficiently Liouville gives NOT strong mixing by these foliations. Actually C^0 rigid.
Some directions of future work:
Herman asks: If \alpha is diophantine, must \phi be conjugate to a rotation?
2010: Fayad-Kritoriam, answer is yes if \phi is globally close to to a rotation. (Close in C^k norm for a value that depends on the
diophantine order of \alpha)
Answers to questions I asked him:
- removing rotation condition is actually delicate. It involves some approximations due to Herman for circle diffeos, and is nontrivial.
- Liouville condition comes in only when he proves the lack of strong
mixing. This is somehow related to showing the foliation is translation invt.
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