Erwin Schrödinger Institute for Mathematical Physics, Vienna, Austria
   
  Semester: Hyperbolic Dynamical Systems
   
  May 25 - July 6, 2008
   
   
   
 



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Motivation (excerpts from the proposal accepted in January 2006)

In many ways, the present semester at ESI is a continuation of a similar effort at ESI in 1996. Then, the main hope was that new progress could be made through the discovery of common threads that run through the analyses of quite different systems such as the Henon map or billiards. In some sense, Lai-Sang Young's 1998 Annals of Math. paper [Y] represents an embodiment of this program.

Since then, techniques from different topics and directions have merged, leading to radically new developments in non-uniformly hyperbolic and partially hyperbolic systems, in hyperbolic systems with singularities, in "large" dynamical systems such as coupled map lattices, and in the application of dynamical systems ideas to nonequilibrium statistical mechanics. There have been spectacular results in the field, where, in particular, we refer to Refs. [D], [Sim2], [T], and to Refs. [WY], [ChD].

We believe that it is time to consolidate these gains and to explore future directions. The new techniques involve a variety of novel ideas and are so elaborate that only a joint effort of the leading experts seems to be able to master them. The trimester at ESI is expected to provide a platform for such a collaborative effort.

Much of the success of the 1996 semester was derived from its interdisciplinary character. Approximately one third of the participants were physicists. We wish to continue in this tradition and intend to bring together researchers in the theory of hyperbolic dynamics and experts in computational dynamics and statistical physics.

Problems to focus on in the ESI semester:

Here, we list some directions in which we expect that progress will be made.

1. Multidimensional Sinai billiards: Chernov generalized Young's ideas on Markov extensions [Y] to multidimensional Anosov systems with singularities. However, this generalization does not cover Sinai billiards where, close to the singularities, the derivative becomes unbounded. As observed by Bálint, Chernov, Szász, and Tóth [BChSzT], this unboundedness leads to the nondifferentiability of the images of the singularities in dimension d ≥3, circumstances that have so far blocked the generalization of Young's construction and, consequently, the control of correlation decay for multidimensional Sinai billiards. Since all other ingredients of hyperbolic theory needed for this task are under control, this is the only remaining obstacle.

2. Semi-dispersing billiards: Success in the previous problem may be followed by results on the control of correlation decay for semi-dispersing billiards. On the level of local ergodicity, a striking problem is to generalize the local ergodicity theorem to the smooth case by dropping the unpleasant algebraicity condition.
An encouraging step forward is the extension of the local ergodicity theorem to certain smooth dispersing billiards by [Bat], [BF] .

3. Ergodicity of hard balls: Simányi's proof of the ergodicity for typical hard ball systems in arbitrary dimensions needs to be simplified in order to obtain a proof of ergodicity of hard ball systems in full generality. Then, there is the problem of balls in a box.

4. Hyperbolic flows with singularities: Improvements of Dolgopyat's methods for the stochastic properties of hyperbolic flows with singularities (including billiard flows) seem now to be within reach.

5. Billiards defined by potentials: It is known that ergodic potentials are exceptional. It is a challenge to find such potentials in higher dimensions, generalizing the 2-dimensional results of Donnay-Liverani. The recent works of Bálint and Tóth aim in that direction.

6. Mechanical models with rotating disks: A new class of mechanical models involving the interaction of particles with rotating disks was introduced [LLM], which involves the exchange of energy between translational and rotational degrees of freedom. From the technical point of view, depending on the ratio of the masses of the disks and particles, these models may have varying degrees of hyperbolicity, but they are not uniformly hyperbolic. Deciphering their statistical properties poses new challenges for billiard techniques.

7. Mechanical models of Brownian motion: It is evident that the ideas and methods of Ref. [ChD] provide fundamental new insights. By their deeper and - hopefully - simplified understanding, it is reasonable to expect that the methods can be extended beyond the limitations of their present conditions, and to other instructive models as well.

8. Rank one attractors: These ideas grew out of earlier work on Hénon maps. By framing the ideas in terms of rank-one maps (i.e. maps with a single direction of instability and strong contraction in all other directions), Wang and Young identified a tractable class of strange attractors that arise naturally. It remains to develop a fuller dynamical picture of these maps, including their geometric and statistical properties, and to establish their presence in various natural physical and mechanical systems defined by ODEs and PDEs.

9. Coupled map lattices: While the situation involving weakly coupled hyperbolic maps is now relatively clear, much remains to be understood in situations where the coupling strength is stronger (but not strong enough for synchronization to occur), and in situations where the constituent maps are not uniformly hyperbolic.

10. Nonequilibrium dynamics: A class of problems related to those above has to do with generalized conduction or transport. As an example we mention chains of coupled particles, where the ends of the chain are connected to heat baths (thermostats) leading to a flow of particles and/or energy along the chain.
Among the questions of interest are the existence of (linear) temperature profiles and descriptions of the particle density along the chain. In Ref. [EY], models similar to those in Ref. [LLM] were studied (see item 6). Stochastic and time-reversible boundaries were used. Problems abound in this area. Such systems play a crucial role in the current revival of nonequilibrium statistical mechanics [RB].

11. Comupter-assisted studies: In addition to the use of computer explorations to give insight into those parts of nonlinear dynamics not (yet) accessible to analytic studies, computer assisted methods can be used to resolve many questions in dynamical systems on a more rigorous level. For example, the presence of Shilnikov-type homoclinic orbits may be verified and the statistical properties of the attractors near them investigated.

12. Theoretical justifications of computations in dynamics: There is an urgent need to better understand the theoretical background and meaning of numerical simulations (see e.g. the Refs. [K], [DSz], and [FL] )

13. Infinite hyperbolic dynamics: There is strong physical motivation for understanding  infinite measure hyperbolic dynamical systems, in particular, the Lorentz process. For recent progress in this direction see, for example, [SzV] and related works.


Bibliography:

[BChSzT] P. Bálint and N. Chernov and D. Szász and I. P. Tóth, Geometry of multidimensional dispersing billiards, Astérisque, 286, 119-150 (2003).

[Bat] P. Batchourine, On the structure of the singularity manifolds of dispersing billiards, arXiv:math/0505620

[BF] P. Batchourine and Ch. Fefferman, The volume near the zeroes of a smooth function, preprint.

[ChD] N. Chernov and D. Dolgopyat, Brownian motion I. manuscript, pp. 192, 2005.

[D] D. Dolgopyat, On decay of correlations in Anosov flows, Ann. of Math., 147, 357-390 (1998).

[DSz] G. Domokos and D. Szász, Ulam's Scheme Revisited: Digital Modeling of Chaotic Attractors via Micro-Perturbations, Discrete and Continuous Dyn. Systems, Ser. A. 9, 859-876 (2003).

[EY] J.-P. Eckmann and L.-S. Young, Temperature profiles in Hamiltonian heat conduction, Europhys. Lett. 68,790-796 (2004).

[FL] P. P. Flockermann, Discretizations of expanding maps, PhD thesis, Dept. of Math., ETH-Zurich] , 2001; and a paper in preparation, with the same title, by P. P. Flockermann and O. E. Lanford

[K] Yu. Kifer, Computations in dynamical systems via random pertubations.
Discrete and Continuous Dyn. Systems, 3, 457-476 (1997).

[LLM] H. Larralde, F. Leyvraz, C. Mejia-Monasterio, Transport properties of a modified Lorentz gas, J. Stat. Phys. 113, 197 (2003).

[RB] L. Rey-Bellet, Statistical mechanics of anharmonic lattices, Contemporary Matheamtics , arXiv:math/0303021.

[Sim2] N. Simányi, The Boltzmann-Sinai ergodic hypothesis in full generality
(without exceptional models)
, arXiv:math/0510022.

[SzV] D. Szász , T Varjú, Local limit theorem for the Lorentz process and its recurrence on the plane, Ergodic Theory and Dynamical Systems (2004), 24, 257-278

[T] W. Tucker, A Rigorous ODE Solver and Smale's 14th Problem,
Found. Comput. Math., 2, 53-117 (2002).

[WY] Q. Wang, L.-S. Young, Toward a theory of rank-one attractors, to appear in Annals of Math.

[Y] L.-S. Young, Statistical properties of systems with some hyperbolicity
including certain biliards
, Ann. of Math., 147, 585-650 (1998).