2016
DOI: 10.1016/j.jde.2016.04.006
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SRB measures for a class of partially hyperbolic attractors in Hilbert spaces

Abstract: In this paper, we study the existence of SRB measures and their properties for infinite dimensional dynamical systems in a Hilbert space. We show several results including (i) if the system has a partially hyperbolic attractor with nontrivial finite dimensional unstable directions, then it has at least one SRB measure; (ii) if the attractor is uniformly hyperbolic and the system is topological mixing and the splitting is Hölder continuous, then there exists a unique SRB measure which is mixing; (iii) if the at… Show more

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Cited by 19 publications
(5 citation statements)
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“…Examples where Assumption 4 is satisfied include: (i) ergodic flows on compact manifolds with Lebesgue absolutely continuous, fully supported, invariant measures, in which case U = V = B µ = M = X; (ii) certain classes of dissipative flows on potentially noncompact manifolds (e.g., the Lorenz 63 (L63) system on M = R 3 [45] studied in Section 8 ahead); and (iii) certain classes of dissipative partial differential equations possessing inertial manifolds and physical measures [44,46].…”
Section: Physical Measuresmentioning
confidence: 99%
“…Examples where Assumption 4 is satisfied include: (i) ergodic flows on compact manifolds with Lebesgue absolutely continuous, fully supported, invariant measures, in which case U = V = B µ = M = X; (ii) certain classes of dissipative flows on potentially noncompact manifolds (e.g., the Lorenz 63 (L63) system on M = R 3 [45] studied in Section 8 ahead); and (iii) certain classes of dissipative partial differential equations possessing inertial manifolds and physical measures [44,46].…”
Section: Physical Measuresmentioning
confidence: 99%
“…As stated in Section 5.2, for data-driven approximation purposes, we will formally assume that the measure µ is physical. While, to our knowledge, there are no results in the literature addressing the existence of physical measures (with appropriate modifications to account for the infinite state space dimension) specifically for the KS system, recent results [63,64] on infinite-dimensional dynamical systems that include the class of dissipative systems in which the KS system belongs indicate that analogs of the assumptions made in Section 5.2 should hold.…”
Section: Overview Of the Kuramoto Sivashinsky Modelmentioning
confidence: 99%
“…Our proof follows in outline the one sketched in [20], and is different than [16,15,9]. We mention that [9], as well as the very recent paper [10], both prove a similar result for mappings of Hilbert spaces. An important difference between Hilbert and Banach spaces is that the latter need not have good geometry.…”
Section: Introduction and Settingmentioning
confidence: 85%
“…We fix δ ≤ 1 4 δ ′ 1 small enough for the results in Section 3 to apply. Let ǫ 0 > 0 is as in Lemma 3.8, and let S be the stack of strong stable leaves defined as in (10)…”
Section: Theorem A: Precise Formulation and Outline Of Proofmentioning
confidence: 99%