Enrique R. Pujals enrique@impa · different backgrounds... Robust and generic dynamics Enrique R....

192
Robust and generic dynamics Enrique R. Pujals [email protected] May 2011, SIAM Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 1 / 29

Transcript of Enrique R. Pujals enrique@impa · different backgrounds... Robust and generic dynamics Enrique R....

  • different backgrounds...

    Robust and generic dynamics

    Enrique R. [email protected]

    May 2011, SIAM

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 1 / 29

  • different backgrounds...

    Setting

    Continuous dynamics

    ẋ = F (x)

    t → Φt (x)

    Discrete dynamics

    Smooth map, f : M → M, where M is a smooth compact manifold

    x f (x) f 2(x) · · · f n(x) f n+1(x)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 2 / 29

  • different backgrounds...

    Setting

    Continuous dynamics

    ẋ = F (x)

    t → Φt (x)

    Discrete dynamics

    Smooth map, f : M → M, where M is a smooth compact manifold

    x f (x) f 2(x) · · · f n(x) f n+1(x)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 2 / 29

  • different backgrounds...

    Setting

    Continuous dynamics

    ẋ = F (x)

    t → Φt (x)

    Discrete dynamics

    Smooth map, f : M → M, where M is a smooth compact manifold

    x f (x) f 2(x) · · · f n(x) f n+1(x)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 2 / 29

  • different backgrounds...

    Setting

    Continuous dynamics

    ẋ = F (x)

    t → Φt (x)

    Discrete dynamics

    Smooth map, f : M → M, where M is a smooth compact manifold

    x f (x) f 2(x) · · · f n(x) f n+1(x)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 2 / 29

  • different backgrounds...

    Setting

    Continuous dynamics

    ẋ = F (x)

    t → Φt (x)

    Discrete dynamics

    Smooth map, f : M → M, where M is a smooth compact manifold

    x f (x) f 2(x) · · · f n(x) f n+1(x)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 2 / 29

  • different backgrounds...

    Setting

    Continuous dynamics

    ẋ = F (x)

    t → Φt (x)

    Discrete dynamics

    Smooth map, f : M → M, where M is a smooth compact manifold

    x f (x) f 2(x) · · · f n(x) f n+1(x)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 2 / 29

  • different backgrounds...

    Setting

    Continuous dynamics

    ẋ = F (x)

    t → Φt (x)

    Discrete dynamics

    Smooth map, f : M → M, where M is a smooth compact manifold

    x f (x) f 2(x) · · · f n(x) f n+1(x)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 2 / 29

  • different backgrounds...

    Goal

    We can “compute the trajectories“ “to describe the dynamics”

    Existence of periodic trajectories?Assymptotic behavior of the trajectories? attractors?“chaotic”?

    Can we trust what we get from numerical approximation?

    How do we interpret the numerical solutions?

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 3 / 29

  • different backgrounds...

    Goal

    We can “compute the trajectories“ “to describe the dynamics”

    Existence of periodic trajectories?Assymptotic behavior of the trajectories? attractors?“chaotic”?

    Can we trust what we get from numerical approximation?

    How do we interpret the numerical solutions?

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 3 / 29

  • different backgrounds...

    Goal

    We can “compute the trajectories“ “to describe the dynamics”

    Existence of periodic trajectories?

    Assymptotic behavior of the trajectories? attractors?“chaotic”?

    Can we trust what we get from numerical approximation?

    How do we interpret the numerical solutions?

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 3 / 29

  • different backgrounds...

    Goal

    We can “compute the trajectories“ “to describe the dynamics”

    Existence of periodic trajectories?Assymptotic behavior of the trajectories? attractors?

    “chaotic”?

    Can we trust what we get from numerical approximation?

    How do we interpret the numerical solutions?

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 3 / 29

  • different backgrounds...

    Goal

    We can “compute the trajectories“ “to describe the dynamics”

    Existence of periodic trajectories?Assymptotic behavior of the trajectories? attractors?“chaotic”?

    Can we trust what we get from numerical approximation?

    How do we interpret the numerical solutions?

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 3 / 29

  • different backgrounds...

    Goal

    We can “compute the trajectories“ “to describe the dynamics”

    Existence of periodic trajectories?Assymptotic behavior of the trajectories? attractors?“chaotic”?

    Can we trust what we get from numerical approximation?

    How do we interpret the numerical solutions?

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 3 / 29

  • different backgrounds...

    Goal

    We can “compute the trajectories“ “to describe the dynamics”

    Existence of periodic trajectories?Assymptotic behavior of the trajectories? attractors?“chaotic”?

    Can we trust what we get from numerical approximation?

    How do we interpret the numerical solutions?

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 3 / 29

  • different backgrounds...

    A taxonomy could help

    “A CLASSIFICATION of possible dynamics”would help to interpret the results

    A “TAXONOMY“ of generic well described dynamical behaviors

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 4 / 29

  • different backgrounds...

    A taxonomy could help

    “A CLASSIFICATION of possible dynamics”would help to interpret the results

    A “TAXONOMY“ of generic well described dynamical behaviors

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 4 / 29

  • different backgrounds...

    A taxonomy could help

    “A CLASSIFICATION of possible dynamics”would help to interpret the results

    A “TAXONOMY“ of generic well described dynamical behaviors

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 4 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“

    Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations

    Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones)

    in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory

    in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.

    GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.

    Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically,

    built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    “How to get a Taxonomy”

    Looking for the possible generic dynamical scenario

    “MODEL OF THE MODELS”

    “Reality to be understood“ Mathematical Models.

    Dynamical Equations Model of those Mathematical Models

    (C. Jones) in theory in delirium (?)

    Properties requiere to those Model of models:

    DYNAMICALLY WELL DESCRIBED.GENERIC.Easy to treat analytically, built “geometrically”.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 5 / 29

  • different backgrounds...

    How to get those model of the models? Example.

    Poincaré and 3 body problem3 bodies interacting under their gravitational attraction.

    2 body problem/Keplerian problem.

    Elliptic motions. Motions are periodic.

    Poincaré: 3 body problem as a perturbation of the 2 body one.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 6 / 29

  • different backgrounds...

    How to get those model of the models? Example.

    Poincaré and 3 body problem

    3 bodies interacting under their gravitational attraction.

    2 body problem/Keplerian problem.

    Elliptic motions. Motions are periodic.

    Poincaré: 3 body problem as a perturbation of the 2 body one.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 6 / 29

  • different backgrounds...

    How to get those model of the models? Example.

    Poincaré and 3 body problem3 bodies interacting under their gravitational attraction.

    2 body problem/Keplerian problem.

    Elliptic motions. Motions are periodic.

    Poincaré: 3 body problem as a perturbation of the 2 body one.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 6 / 29

  • different backgrounds...

    How to get those model of the models? Example.

    Poincaré and 3 body problem3 bodies interacting under their gravitational attraction.

    2 body problem/Keplerian problem.

    Elliptic motions. Motions are periodic.

    Poincaré: 3 body problem as a perturbation of the 2 body one.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 6 / 29

  • different backgrounds...

    How to get those model of the models? Example.

    Poincaré and 3 body problem3 bodies interacting under their gravitational attraction.

    2 body problem/Keplerian problem.

    Elliptic motions. Motions are periodic.

    Poincaré: 3 body problem as a perturbation of the 2 body one.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 6 / 29

  • different backgrounds...

    How to get those model of the models? Example.

    Poincaré and 3 body problem3 bodies interacting under their gravitational attraction.

    2 body problem/Keplerian problem.

    Elliptic motions. Motions are periodic.

    Poincaré: 3 body problem as a perturbation of the 2 body one.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 6 / 29

  • different backgrounds...

    How to get those model of the models? Example.

    Poincaré and 3 body problem3 bodies interacting under their gravitational attraction.

    2 body problem/Keplerian problem.

    Elliptic motions.

    Motions are periodic.

    Poincaré: 3 body problem as a perturbation of the 2 body one.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 6 / 29

  • different backgrounds...

    How to get those model of the models? Example.

    Poincaré and 3 body problem3 bodies interacting under their gravitational attraction.

    2 body problem/Keplerian problem.

    Elliptic motions. Motions are periodic.

    Poincaré: 3 body problem as a perturbation of the 2 body one.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 6 / 29

  • different backgrounds...

    How to get those model of the models? Example.

    Poincaré and 3 body problem3 bodies interacting under their gravitational attraction.

    2 body problem/Keplerian problem.

    Elliptic motions. Motions are periodic.

    Poincaré: 3 body problem as a perturbation of the 2 body one.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 6 / 29

  • different backgrounds...

    3 body problem.

    Poincaré observed “complicated trajectories”.

    “...One will be struck by the complexity of this figure, which I am noteven attempting to draw.”

    “...Nothing can give us a better idea of the intricacy of the three-bodyproblem....”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 7 / 29

  • different backgrounds...

    3 body problem.

    Poincaré observed “complicated trajectories”.

    “...One will be struck by the complexity of this figure, which I am noteven attempting to draw.”

    “...Nothing can give us a better idea of the intricacy of the three-bodyproblem....”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 7 / 29

  • different backgrounds...

    3 body problem.

    Poincaré observed “complicated trajectories”.

    “...One will be struck by the complexity of this figure, which I am noteven attempting to draw.”

    “...Nothing can give us a better idea of the intricacy of the three-bodyproblem....”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 7 / 29

  • different backgrounds...

    3 body problem.

    Poincaré observed “complicated trajectories”.

    “...One will be struck by the complexity of this figure, which I am noteven attempting to draw.”

    “...Nothing can give us a better idea of the intricacy of the three-bodyproblem....”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 7 / 29

  • different backgrounds...

    3 body problem.

    Poincaré observed “complicated trajectories”.

    “...One will be struck by the complexity of this figure, which I am noteven attempting to draw.”

    “...Nothing can give us a better idea of the intricacy of the three-bodyproblem....”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 7 / 29

  • different backgrounds...

    How is that possible?

    Find a DYNAMICAL CONFIGURATION:

    that provides the dynamical properties that we want;gives more information;

    it is easy to be detected;it is “UNIVERSAL”.

    It can be found in the original problem.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 8 / 29

  • different backgrounds...

    How is that possible?

    Find a DYNAMICAL CONFIGURATION:

    that provides the dynamical properties that we want;gives more information;

    it is easy to be detected;it is “UNIVERSAL”.

    It can be found in the original problem.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 8 / 29

  • different backgrounds...

    How is that possible?

    Find a DYNAMICAL CONFIGURATION:

    that provides the dynamical properties that we want;

    gives more information;

    it is easy to be detected;it is “UNIVERSAL”.

    It can be found in the original problem.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 8 / 29

  • different backgrounds...

    How is that possible?

    Find a DYNAMICAL CONFIGURATION:

    that provides the dynamical properties that we want;gives more information;

    it is easy to be detected;it is “UNIVERSAL”.

    It can be found in the original problem.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 8 / 29

  • different backgrounds...

    How is that possible?

    Find a DYNAMICAL CONFIGURATION:

    that provides the dynamical properties that we want;gives more information;

    it is easy to be detected;

    it is “UNIVERSAL”.

    It can be found in the original problem.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 8 / 29

  • different backgrounds...

    How is that possible?

    Find a DYNAMICAL CONFIGURATION:

    that provides the dynamical properties that we want;gives more information;

    it is easy to be detected;it is “UNIVERSAL”.

    It can be found in the original problem.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 8 / 29

  • different backgrounds...

    How is that possible?

    Find a DYNAMICAL CONFIGURATION:

    that provides the dynamical properties that we want;gives more information;

    it is easy to be detected;it is “UNIVERSAL”.

    It can be found in the original problem.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 8 / 29

  • different backgrounds...

    Poincaré: Homoclinic points.

    Homoclinic points: “Points with same past and future"

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 9 / 29

  • different backgrounds...

    Poincaré: Homoclinic points.

    Homoclinic points: “Points with same past and future"

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 9 / 29

  • different backgrounds...

    Poincaré: Homoclinic points.

    Homoclinic points: “Points with same past and future"

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 9 / 29

  • different backgrounds...

    Poincaré: Homoclinic points.

    Homoclinic points: “Points with same past and future"

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 9 / 29

  • different backgrounds...

    Poincaré: Homoclinic points.

    Homoclinic points: “Points with same past and future"

    Infinitely many periodic orbits.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 9 / 29

  • different backgrounds...

    Poincaré: Homoclinic points.

    Homoclinic points: “Points with same past and future"

    Infinitely many periodic orbits.

    Chaotic dynamic.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 9 / 29

  • different backgrounds...

    Poincaré: Homoclinic points.

    Homoclinic points: “Points with same past and future"

    Infinitely many periodic orbits.

    Chaotic dynamic.

    It holds in a robust way.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 9 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    Dichotomy

    Either the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE:

    Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable.

    Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point.

    There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Homoclic points.

    Appears in the 3 body problem.

    Perturbed pendulum.

    Generic in mechanical problems with at least two degree of freedom

    DichotomyEither the dynamics is VERY SIMPLE: Integrable. Morse-Smale inthe non-conservative case,

    or there is a transversal homoclinic point. There are chaoticcomponents.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 10 / 29

  • different backgrounds...

    Transv. Hom. points: source of Hyperbolic theory.

    Smale’s Horseshoes:

    Hyperbolic Structure

    TΛM = Es ⊕ Eu

    ||Df/Es || < λ < 1, (squeeze) ||Df−1/Eu || < λ < 1, (strecht)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 11 / 29

  • different backgrounds...

    Transv. Hom. points: source of Hyperbolic theory.

    Smale’s Horseshoes:

    Hyperbolic Structure

    TΛM = Es ⊕ Eu

    ||Df/Es || < λ < 1, (squeeze) ||Df−1/Eu || < λ < 1, (strecht)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 11 / 29

  • different backgrounds...

    Transv. Hom. points: source of Hyperbolic theory.

    Smale’s Horseshoes:

    Hyperbolic Structure

    TΛM = Es ⊕ Eu

    ||Df/Es || < λ < 1, (squeeze) ||Df−1/Eu || < λ < 1, (strecht)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 11 / 29

  • different backgrounds...

    Transv. Hom. points: source of Hyperbolic theory.

    Smale’s Horseshoes:

    Hyperbolic Structure

    TΛM = Es ⊕ Eu

    ||Df/Es || < λ < 1, (squeeze) ||Df−1/Eu || < λ < 1, (strecht)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 11 / 29

  • different backgrounds...

    Transv. Hom. points: source of Hyperbolic theory.

    Smale’s Horseshoes:

    Hyperbolic Structure

    TΛM = Es ⊕ Eu

    ||Df/Es || < λ < 1, (squeeze) ||Df−1/Eu || < λ < 1, (strecht)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 11 / 29

  • different backgrounds...

    Transv. Hom. points: source of Hyperbolic theory.

    Smale’s Horseshoes:

    Hyperbolic Structure

    TΛM = Es ⊕ Eu

    ||Df/Es || < λ < 1, (squeeze) ||Df−1/Eu || < λ < 1, (strecht)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 11 / 29

  • different backgrounds...

    Transv. Hom. points: source of Hyperbolic theory.

    Smale’s Horseshoes:

    Hyperbolic Structure

    TΛM = Es ⊕ Eu

    ||Df/Es || < λ < 1, (squeeze) ||Df−1/Eu || < λ < 1, (strecht)

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 11 / 29

  • different backgrounds...

    Nice description of Hyperbolic systems

    ROBUST CHAOTIC dynamics.

    ROBUST TRANSITIVE dynamics.

    1 Infinitely many periodic orbits,2 Stable systems;3 Nice statistical properties.

    NICE PICTURE FOR HYPERBOLIC SYSTEMS

    Hyperbolicity, a happy story.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 12 / 29

  • different backgrounds...

    Nice description of Hyperbolic systems

    ROBUST CHAOTIC dynamics.

    ROBUST TRANSITIVE dynamics.

    1 Infinitely many periodic orbits,2 Stable systems;3 Nice statistical properties.

    NICE PICTURE FOR HYPERBOLIC SYSTEMS

    Hyperbolicity, a happy story.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 12 / 29

  • different backgrounds...

    Nice description of Hyperbolic systems

    ROBUST CHAOTIC dynamics.

    ROBUST TRANSITIVE dynamics.

    1 Infinitely many periodic orbits,2 Stable systems;3 Nice statistical properties.

    NICE PICTURE FOR HYPERBOLIC SYSTEMS

    Hyperbolicity, a happy story.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 12 / 29

  • different backgrounds...

    Nice description of Hyperbolic systems

    ROBUST CHAOTIC dynamics.

    ROBUST TRANSITIVE dynamics.

    1 Infinitely many periodic orbits,

    2 Stable systems;3 Nice statistical properties.

    NICE PICTURE FOR HYPERBOLIC SYSTEMS

    Hyperbolicity, a happy story.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 12 / 29

  • different backgrounds...

    Nice description of Hyperbolic systems

    ROBUST CHAOTIC dynamics.

    ROBUST TRANSITIVE dynamics.

    1 Infinitely many periodic orbits,2 Stable systems;

    3 Nice statistical properties.

    NICE PICTURE FOR HYPERBOLIC SYSTEMS

    Hyperbolicity, a happy story.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 12 / 29

  • different backgrounds...

    Nice description of Hyperbolic systems

    ROBUST CHAOTIC dynamics.

    ROBUST TRANSITIVE dynamics.

    1 Infinitely many periodic orbits,2 Stable systems;3 Nice statistical properties.

    NICE PICTURE FOR HYPERBOLIC SYSTEMS

    Hyperbolicity, a happy story.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 12 / 29

  • different backgrounds...

    Nice description of Hyperbolic systems

    ROBUST CHAOTIC dynamics.

    ROBUST TRANSITIVE dynamics.

    1 Infinitely many periodic orbits,2 Stable systems;3 Nice statistical properties.

    NICE PICTURE FOR HYPERBOLIC SYSTEMS

    Hyperbolicity, a happy story.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 12 / 29

  • different backgrounds...

    Nice description of Hyperbolic systems

    ROBUST CHAOTIC dynamics.

    ROBUST TRANSITIVE dynamics.

    1 Infinitely many periodic orbits,2 Stable systems;3 Nice statistical properties.

    NICE PICTURE FOR HYPERBOLIC SYSTEMS

    Hyperbolicity, a happy story.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 12 / 29

  • different backgrounds...

    Mechanical examples of Hyperbolic systems

    The triple linkage

    Geodesic flow in a manifold of negative curvature (Hunt-MacKay).

    GLOBAL HYPERBOLIC FLOW.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 13 / 29

  • different backgrounds...

    Mechanical examples of Hyperbolic systemsThe triple linkage

    Geodesic flow in a manifold of negative curvature (Hunt-MacKay).

    GLOBAL HYPERBOLIC FLOW.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 13 / 29

  • different backgrounds...

    Mechanical examples of Hyperbolic systemsThe triple linkage

    Geodesic flow in a manifold of negative curvature (Hunt-MacKay).

    GLOBAL HYPERBOLIC FLOW.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 13 / 29

  • different backgrounds...

    Mechanical examples of Hyperbolic systemsThe triple linkage

    Geodesic flow in a manifold of negative curvature (Hunt-MacKay).

    GLOBAL HYPERBOLIC FLOW.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 13 / 29

  • different backgrounds...

    Mechanical examples of Hyperbolic systemsThe triple linkage

    Geodesic flow in a manifold of negative curvature (Hunt-MacKay).

    GLOBAL HYPERBOLIC FLOW.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 13 / 29

  • different backgrounds...

    Mechanical examples of Hyperbolic systemsThe triple linkage

    Geodesic flow in a manifold of negative curvature (Hunt-MacKay).

    GLOBAL HYPERBOLIC FLOW.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 13 / 29

  • different backgrounds...

    ”Robust” implies Hyperbolicity?

    There are robust dynamics which are not hyperbolic

    Only in higher dimension

    For surfaces: Robust chaotic dynamics —-> Hyperbolicity.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 14 / 29

  • different backgrounds...

    ”Robust” implies Hyperbolicity?

    There are robust dynamics which are not hyperbolic

    Only in higher dimension

    For surfaces: Robust chaotic dynamics —-> Hyperbolicity.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 14 / 29

  • different backgrounds...

    ”Robust” implies Hyperbolicity?

    There are robust dynamics which are not hyperbolic

    Only in higher dimension

    For surfaces: Robust chaotic dynamics —-> Hyperbolicity.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 14 / 29

  • different backgrounds...

    ”Robust” implies Hyperbolicity?

    There are robust dynamics which are not hyperbolic

    Only in higher dimension

    For surfaces: Robust chaotic dynamics

    —-> Hyperbolicity.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 14 / 29

  • different backgrounds...

    ”Robust” implies Hyperbolicity?

    There are robust dynamics which are not hyperbolic

    Only in higher dimension

    For surfaces: Robust chaotic dynamics —-> Hyperbolicity.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 14 / 29

  • different backgrounds...

    Non-Hyperbolic Robust transitive systems.

    1 take f : M2 → M2 Hyperbolic diffeo;2 take g : N2 → N2 be either an integrable one (pendulum/forced

    pendulum);

    f × g : M2 × N2 → M2 × N2.

    PARTIAL HYPERBOLICITY

    Arnold’s diffusion

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 15 / 29

  • different backgrounds...

    Non-Hyperbolic Robust transitive systems.

    1 take f : M2 → M2 Hyperbolic diffeo;

    2 take g : N2 → N2 be either an integrable one (pendulum/forcedpendulum);

    f × g : M2 × N2 → M2 × N2.

    PARTIAL HYPERBOLICITY

    Arnold’s diffusion

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 15 / 29

  • different backgrounds...

    Non-Hyperbolic Robust transitive systems.

    1 take f : M2 → M2 Hyperbolic diffeo;2 take g : N2 → N2 be either an integrable one (pendulum/forced

    pendulum);

    f × g : M2 × N2 → M2 × N2.

    PARTIAL HYPERBOLICITY

    Arnold’s diffusion

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 15 / 29

  • different backgrounds...

    Non-Hyperbolic Robust transitive systems.

    1 take f : M2 → M2 Hyperbolic diffeo;2 take g : N2 → N2 be either an integrable one (pendulum/forced

    pendulum);

    f × g : M2 × N2 → M2 × N2.

    PARTIAL HYPERBOLICITY

    Arnold’s diffusion

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 15 / 29

  • different backgrounds...

    Non-Hyperbolic Robust transitive systems.

    1 take f : M2 → M2 Hyperbolic diffeo;2 take g : N2 → N2 be either an integrable one (pendulum/forced

    pendulum);

    f × g : M2 × N2 → M2 × N2.

    PARTIAL HYPERBOLICITY

    Arnold’s diffusion

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 15 / 29

  • different backgrounds...

    Non-Hyperbolic Robust transitive systems.

    1 take f : M2 → M2 Hyperbolic diffeo;2 take g : N2 → N2 be either an integrable one (pendulum/forced

    pendulum);

    f × g : M2 × N2 → M2 × N2.

    PARTIAL HYPERBOLICITY

    Arnold’s diffusion

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 15 / 29

  • different backgrounds...

    Non-Hyperbolic Robust transitive systems.

    1 take f : M2 → M2 Hyperbolic diffeo;2 take g : N2 → N2 be either an integrable one (pendulum/forced

    pendulum);

    f × g : M2 × N2 → M2 × N2.

    PARTIAL HYPERBOLICITY

    Arnold’s diffusion

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 15 / 29

  • different backgrounds...

    Non-Hyperbolic Robust transitive systems.

    1 take f : M2 → M2 Hyperbolic diffeo;2 take g : N2 → N2 be either an integrable one (pendulum/forced

    pendulum);

    f × g : M2 × N2 → M2 × N2.

    PARTIAL HYPERBOLICITY

    Arnold’s diffusion

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 15 / 29

  • different backgrounds...

    Robust dynamic for flows: Lorenz Attractor

    X (x , y , z) =

    ẋ = −αx + αyẏ = βx − y − xzż = −γz + xy ,

    Lorenz: for parameters close to 10,28,8/3 there is a RobustTransitive Attractor containing a singularity (equilibrium point).

    Presences of singularity prevents the hyperbolicity

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 16 / 29

  • different backgrounds...

    Robust dynamic for flows: Lorenz Attractor

    X (x , y , z) =

    ẋ = −αx + αyẏ = βx − y − xzż = −γz + xy ,

    Lorenz: for parameters close to 10,28,8/3 there is a RobustTransitive Attractor containing a singularity (equilibrium point).

    Presences of singularity prevents the hyperbolicity

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 16 / 29

  • different backgrounds...

    Robust dynamic for flows: Lorenz Attractor

    X (x , y , z) =

    ẋ = −αx + αyẏ = βx − y − xzż = −γz + xy ,

    Lorenz: for parameters close to 10,28,8/3 there is a RobustTransitive Attractor containing a singularity (equilibrium point).

    Presences of singularity prevents the hyperbolicity

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 16 / 29

  • different backgrounds...

    Robust dynamic for flows: Lorenz Attractor

    X (x , y , z) =

    ẋ = −αx + αyẏ = βx − y − xzż = −γz + xy ,

    Lorenz: for parameters close to 10,28,8/3 there is a RobustTransitive Attractor containing a singularity (equilibrium point).

    Presences of singularity prevents the hyperbolicity

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 16 / 29

  • different backgrounds...

    Geometric Lorenz attractors

    Geometric models of robust transitive attractor with singularities(Guckenheimer-Williams).

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 17 / 29

  • different backgrounds...

    Geometric Lorenz attractors

    Geometric models of robust transitive attractor with singularities(Guckenheimer-Williams).

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 17 / 29

  • different backgrounds...

    Geometric Lorenz attractors

    Geometric models of robust transitive attractor with singularities(Guckenheimer-Williams).

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 17 / 29

  • different backgrounds...

    Singular Hyperbolicity

    Structure underlying the GLA

    TΛ = Es ⊕ Ecu,

    Rich dynamic obtained from Singular hyperbolicity:1 Density of periodic orbits/ chaoticity;2 Good statistical properties.

    Lorenz’s equation is a Geometric Lorenz Attractor

    Any C1−robust attractor with singularitiesis a Geometric Lorenz Attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 18 / 29

  • different backgrounds...

    Singular Hyperbolicity

    Structure underlying the GLA

    TΛ = Es ⊕ Ecu,

    Rich dynamic obtained from Singular hyperbolicity:1 Density of periodic orbits/ chaoticity;2 Good statistical properties.

    Lorenz’s equation is a Geometric Lorenz Attractor

    Any C1−robust attractor with singularitiesis a Geometric Lorenz Attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 18 / 29

  • different backgrounds...

    Singular Hyperbolicity

    Structure underlying the GLA

    TΛ = Es ⊕ Ecu,

    Rich dynamic obtained from Singular hyperbolicity:1 Density of periodic orbits/ chaoticity;2 Good statistical properties.

    Lorenz’s equation is a Geometric Lorenz Attractor

    Any C1−robust attractor with singularitiesis a Geometric Lorenz Attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 18 / 29

  • different backgrounds...

    Singular Hyperbolicity

    Structure underlying the GLA

    TΛ = Es ⊕ Ecu,

    Rich dynamic obtained from Singular hyperbolicity:

    1 Density of periodic orbits/ chaoticity;2 Good statistical properties.

    Lorenz’s equation is a Geometric Lorenz Attractor

    Any C1−robust attractor with singularitiesis a Geometric Lorenz Attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 18 / 29

  • different backgrounds...

    Singular Hyperbolicity

    Structure underlying the GLA

    TΛ = Es ⊕ Ecu,

    Rich dynamic obtained from Singular hyperbolicity:1 Density of periodic orbits/ chaoticity;

    2 Good statistical properties.

    Lorenz’s equation is a Geometric Lorenz Attractor

    Any C1−robust attractor with singularitiesis a Geometric Lorenz Attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 18 / 29

  • different backgrounds...

    Singular Hyperbolicity

    Structure underlying the GLA

    TΛ = Es ⊕ Ecu,

    Rich dynamic obtained from Singular hyperbolicity:1 Density of periodic orbits/ chaoticity;2 Good statistical properties.

    Lorenz’s equation is a Geometric Lorenz Attractor

    Any C1−robust attractor with singularitiesis a Geometric Lorenz Attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 18 / 29

  • different backgrounds...

    Singular Hyperbolicity

    Structure underlying the GLA

    TΛ = Es ⊕ Ecu,

    Rich dynamic obtained from Singular hyperbolicity:1 Density of periodic orbits/ chaoticity;2 Good statistical properties.

    Lorenz’s equation is a Geometric Lorenz Attractor

    Any C1−robust attractor with singularitiesis a Geometric Lorenz Attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 18 / 29

  • different backgrounds...

    Singular Hyperbolicity

    Structure underlying the GLA

    TΛ = Es ⊕ Ecu,

    Rich dynamic obtained from Singular hyperbolicity:1 Density of periodic orbits/ chaoticity;2 Good statistical properties.

    Lorenz’s equation is a Geometric Lorenz Attractor

    Any C1−robust attractor with singularitiesis a Geometric Lorenz Attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 18 / 29

  • different backgrounds...

    Robustness implies structure.

    Can we characterize robust dynamics which are not hyperbolic

    ROBUSTNESS IMPLIES WEAK HYPERBOLICITY.

    NICE DYNAMICAL PROPERTIES (sometimes under extra assumptions)

    Abundance of periodic trajectories;good statistical properties.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 19 / 29

  • different backgrounds...

    Robustness implies structure.

    Can we characterize robust dynamics which are not hyperbolic

    ROBUSTNESS IMPLIES WEAK HYPERBOLICITY.

    NICE DYNAMICAL PROPERTIES (sometimes under extra assumptions)

    Abundance of periodic trajectories;good statistical properties.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 19 / 29

  • different backgrounds...

    Robustness implies structure.

    Can we characterize robust dynamics which are not hyperbolic

    ROBUSTNESS IMPLIES

    WEAK HYPERBOLICITY.

    NICE DYNAMICAL PROPERTIES (sometimes under extra assumptions)

    Abundance of periodic trajectories;good statistical properties.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 19 / 29

  • different backgrounds...

    Robustness implies structure.

    Can we characterize robust dynamics which are not hyperbolic

    ROBUSTNESS IMPLIES WEAK HYPERBOLICITY.

    NICE DYNAMICAL PROPERTIES (sometimes under extra assumptions)

    Abundance of periodic trajectories;good statistical properties.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 19 / 29

  • different backgrounds...

    Robustness implies structure.

    Can we characterize robust dynamics which are not hyperbolic

    ROBUSTNESS IMPLIES WEAK HYPERBOLICITY.

    NICE DYNAMICAL PROPERTIES (sometimes under extra assumptions)

    Abundance of periodic trajectories;good statistical properties.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 19 / 29

  • different backgrounds...

    Robustness implies structure.

    Can we characterize robust dynamics which are not hyperbolic

    ROBUSTNESS IMPLIES WEAK HYPERBOLICITY.

    NICE DYNAMICAL PROPERTIES (sometimes under extra assumptions)

    Abundance of periodic trajectories;

    good statistical properties.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 19 / 29

  • different backgrounds...

    Robustness implies structure.

    Can we characterize robust dynamics which are not hyperbolic

    ROBUSTNESS IMPLIES WEAK HYPERBOLICITY.

    NICE DYNAMICAL PROPERTIES (sometimes under extra assumptions)

    Abundance of periodic trajectories;good statistical properties.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 19 / 29

  • different backgrounds...

    Everything is ”Robust”?

    NO. WILD DYNAMICS.

    Infinitely many attractors apearing and dissapearing

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 20 / 29

  • different backgrounds...

    Everything is ”Robust”?

    NO. WILD DYNAMICS.

    Infinitely many attractors apearing and dissapearing

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 20 / 29

  • different backgrounds...

    Everything is ”Robust”?

    NO. WILD DYNAMICS.

    Infinitely many attractors apearing and dissapearing

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 20 / 29

  • different backgrounds...

    Everything is ”Robust”?

    NO. WILD DYNAMICS.

    Infinitely many attractors apearing and dissapearing

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 20 / 29

  • different backgrounds...

    Everything is ”Robust”?

    NO. WILD DYNAMICS.

    Infinitely many attractors apearing and dissapearing

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 20 / 29

  • different backgrounds...

    Everything is ”Robust”?

    NO. WILD DYNAMICS.

    Infinitely many attractors apearing and dissapearing

    Perturbations of Integrable systems

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 20 / 29

  • different backgrounds...

    Everything is ”Robust”?

    NO. WILD DYNAMICS.

    Infinitely many attractors apearing and dissapearing

    Perturbations of Integrable systems

    New kind of homoclinic pointsEnrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 20 / 29

  • different backgrounds...

    Homoclinic points: Wild dynamics

    Homoclinic points:

    Hyperbolicity=Transversal homoclinic points.

    Breaking Hyperbolicity =Tangent homoclinic points.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 21 / 29

  • different backgrounds...

    Homoclinic points: Wild dynamics

    Homoclinic points:

    Hyperbolicity=Transversal homoclinic points.

    Breaking Hyperbolicity =Tangent homoclinic points.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 21 / 29

  • different backgrounds...

    Homoclinic points: Wild dynamics

    Homoclinic points:

    Hyperbolicity=Transversal homoclinic points.

    Breaking Hyperbolicity =Tangent homoclinic points.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 21 / 29

  • different backgrounds...

    TANGENCIES IMPLY WILD SETS

    Newhouse: Unfolding homoclinic tangencies

    Residual sets of diffeos having infinitely many periodic attractors.

    One tangency —> a cascade of infinitely many tangencies —> infinitelymany periodic attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 22 / 29

  • different backgrounds...

    TANGENCIES IMPLY WILD SETS

    Newhouse: Unfolding homoclinic tangencies

    Residual sets of diffeos having infinitely many periodic attractors.

    One tangency —> a cascade of infinitely many tangencies —> infinitelymany periodic attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 22 / 29

  • different backgrounds...

    TANGENCIES IMPLY WILD SETS

    Newhouse: Unfolding homoclinic tangencies

    Residual sets of diffeos having infinitely many periodic attractors.

    One tangency —>

    a cascade of infinitely many tangencies —> infinitelymany periodic attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 22 / 29

  • different backgrounds...

    TANGENCIES IMPLY WILD SETS

    Newhouse: Unfolding homoclinic tangencies

    Residual sets of diffeos having infinitely many periodic attractors.

    One tangency —> a cascade of infinitely many tangencies —>

    infinitelymany periodic attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 22 / 29

  • different backgrounds...

    TANGENCIES IMPLY WILD SETS

    Newhouse: Unfolding homoclinic tangencies

    Residual sets of diffeos having infinitely many periodic attractors.

    One tangency —> a cascade of infinitely many tangencies —> infinitelymany periodic attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 22 / 29

  • different backgrounds...

    TANGENCIES IMPLY WILD SETS

    Newhouse: Unfolding homoclinic tangencies

    Residual sets of diffeos having infinitely many periodic attractors.

    One tangency —> a cascade of infinitely many tangencies —> infinitelymany periodic attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 22 / 29

  • different backgrounds...

    TANGENCIES IMPLY WILD SETS

    Newhouse: Unfolding homoclinic tangencies

    Residual sets of diffeos having infinitely many periodic attractors.

    One tangency —> a cascade of infinitely many tangencies —> infinitelymany periodic attractor.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 22 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 23 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics

    also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    GENERIC DYNAMICS/UNIVERSAL MECHANISMS

    Coming back to the possible dynamical scenario:

    Robust dynamics also called Tame dynamics

    Wild dynamics

    How can we explain those dynamical behaviors?

    Dictionary?

    Phenomenas/Mechanisms

    Phenomena: Some well described dynamical behavior

    Mechanisms: Some dynamical configuration and its perturbations.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 24 / 29

  • different backgrounds...

    UNIVERSAL MECHANISMS/GENERIC DYNAMICS

    PHENOMENA MECHANISMS

    The collection of phenomenas has to be generic

    The collection of mechanisms has to be simply and generic

    Rich in their consequences

    “HOMOCLINIC BIFURCATIONS should be the MECHANISMS”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 25 / 29

  • different backgrounds...

    UNIVERSAL MECHANISMS/GENERIC DYNAMICS

    PHENOMENA MECHANISMS

    The collection of phenomenas has to be generic

    The collection of mechanisms has to be simply and generic

    Rich in their consequences

    “HOMOCLINIC BIFURCATIONS should be the MECHANISMS”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 25 / 29

  • different backgrounds...

    UNIVERSAL MECHANISMS/GENERIC DYNAMICS

    PHENOMENA MECHANISMS

    The collection of phenomenas has to be generic

    The collection of mechanisms has to be simply and generic

    Rich in their consequences

    “HOMOCLINIC BIFURCATIONS should be the MECHANISMS”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 25 / 29

  • different backgrounds...

    UNIVERSAL MECHANISMS/GENERIC DYNAMICS

    PHENOMENA MECHANISMS

    The collection of phenomenas has to be generic

    The collection of mechanisms has to be simply and generic

    Rich in their consequences

    “HOMOCLINIC BIFURCATIONS should be the MECHANISMS”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 25 / 29

  • different backgrounds...

    UNIVERSAL MECHANISMS/GENERIC DYNAMICS

    PHENOMENA MECHANISMS

    The collection of phenomenas has to be generic

    The collection of mechanisms has to be simply and generic

    Rich in their consequences

    “HOMOCLINIC BIFURCATIONS should be the MECHANISMS”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 25 / 29

  • different backgrounds...

    UNIVERSAL MECHANISMS/GENERIC DYNAMICS

    PHENOMENA MECHANISMS

    The collection of phenomenas has to be generic

    The collection of mechanisms has to be simply and generic

    Rich in their consequences

    “HOMOCLINIC BIFURCATIONS should be the MECHANISMS”

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 25 / 29

  • different backgrounds...

    Dichotomy in low dimension.

    Dynamical dichotomy for low dimension:

    Robust Dynamics = Hyperbolic systems

    Wild dynamic “=” homoclinic tangencies.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 26 / 29

  • different backgrounds...

    Dichotomy in low dimension.

    Dynamical dichotomy for low dimension:

    Robust Dynamics = Hyperbolic systems

    Wild dynamic “=” homoclinic tangencies.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 26 / 29

  • different backgrounds...

    Dichotomy in low dimension.

    Dynamical dichotomy for low dimension:

    Robust Dynamics = Hyperbolic systems

    Wild dynamic “=” homoclinic tangencies.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 26 / 29

  • different backgrounds...

    Dichotomy in low dimension.

    Dynamical dichotomy for low dimension:

    Robust Dynamics = Hyperbolic systems

    Wild dynamic “=” homoclinic tangencies.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 26 / 29

  • different backgrounds...

    What about higher dimensions?

    The situation changes dramatically!!

    The ZOO (phenomenas) is becomes larger.

    There are Robust chaotic dynamics which are NOT hyperbolic.

    New type of wild dynamics.

    New Mechanisms/Homoclinic bifurcations get into the picture.

    Heterodimensional cycle.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 27 / 29

  • different backgrounds...

    What about higher dimensions?

    The situation changes dramatically!!

    The ZOO (phenomenas) is becomes larger.

    There are Robust chaotic dynamics which are NOT hyperbolic.

    New type of wild dynamics.

    New Mechanisms/Homoclinic bifurcations get into the picture.

    Heterodimensional cycle.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 27 / 29

  • different backgrounds...

    What about higher dimensions?

    The situation changes dramatically!!

    The ZOO (phenomenas) is becomes larger.

    There are Robust chaotic dynamics which are NOT hyperbolic.

    New type of wild dynamics.

    New Mechanisms/Homoclinic bifurcations get into the picture.

    Heterodimensional cycle.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 27 / 29

  • different backgrounds...

    What about higher dimensions?

    The situation changes dramatically!!

    The ZOO (phenomenas) is becomes larger.

    There are Robust chaotic dynamics which are NOT hyperbolic.

    New type of wild dynamics.

    New Mechanisms/Homoclinic bifurcations get into the picture.

    Heterodimensional cycle.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 27 / 29

  • different backgrounds...

    What about higher dimensions?

    The situation changes dramatically!!

    The ZOO (phenomenas) is becomes larger.

    There are Robust chaotic dynamics which are NOT hyperbolic.

    New type of wild dynamics.

    New Mechanisms/Homoclinic bifurcations get into the picture.

    Heterodimensional cycle.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 27 / 29

  • different backgrounds...

    What about higher dimensions?

    The situation changes dramatically!!

    The ZOO (phenomenas) is becomes larger.

    There are Robust chaotic dynamics which are NOT hyperbolic.

    New type of wild dynamics.

    New Mechanisms/Homoclinic bifurcations get into the picture.

    Heterodimensional cycle.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 27 / 29

  • different backgrounds...

    What about higher dimensions?

    The situation changes dramatically!!

    The ZOO (phenomenas) is becomes larger.

    There are Robust chaotic dynamics which are NOT hyperbolic.

    New type of wild dynamics.

    New Mechanisms/Homoclinic bifurcations get into the picture.

    Heterodimensional cycle.

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 27 / 29

  • different backgrounds...

    Phenom.Mechanisms/ Dichotomies in any dimen?

    There is reasonable (vague), almost generic list of phenomenas.

    There is reasonable list of mechanisms.

    Some relation between New phenomenas/New mechanisms

    Incomplete dictionary

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 28 / 29

  • different backgrounds...

    Phenom.Mechanisms/ Dichotomies in any dimen?

    There is reasonable (vague), almost generic list of phenomenas.

    There is reasonable list of mechanisms.

    Some relation between New phenomenas/New mechanisms

    Incomplete dictionary

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 28 / 29

  • different backgrounds...

    Phenom.Mechanisms/ Dichotomies in any dimen?

    There is reasonable (vague), almost generic list of phenomenas.

    There is reasonable list of mechanisms.

    Some relation between New phenomenas/New mechanisms

    Incomplete dictionary

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 28 / 29

  • different backgrounds...

    Phenom.Mechanisms/ Dichotomies in any dimen?

    There is reasonable (vague), almost generic list of phenomenas.

    There is reasonable list of mechanisms.

    Some relation between New phenomenas/New mechanisms

    Incomplete dictionary

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 28 / 29

  • different backgrounds...

    Phenom.Mechanisms/ Dichotomies in any dimen?

    There is reasonable (vague), almost generic list of phenomenas.

    There is reasonable list of mechanisms.

    Some relation between New phenomenas/New mechanisms

    Incomplete dictionary

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 28 / 29

  • different backgrounds...

    Phenom.Mechanisms/ Dictionari in any dimen?

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 29 / 29

  • different backgrounds...

    Phenom.Mechanisms/ Dictionari in any dimen?

    Enrique R. Pujals (IMPA) Dynamical Systems SIAM 2011 29 / 29