2021
DOI: 10.3390/e23111405
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Entropy and Ergodicity of Boole-Type Transformations

Abstract: We review some analytic, measure-theoretic and topological techniques for studying ergodicity and entropy of discrete dynamical systems, with a focus on Boole-type transformations and their generalizations. In particular, we present a new proof of the ergodicity of the 1-dimensional Boole map and prove that a certain 2-dimensional generalization is also ergodic. Moreover, we compute and demonstrate the equivalence of metric and topological entropies of the 1-dimensional Boole map employing “compactified”repres… Show more

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Cited by 3 publications
(5 citation statements)
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“…for any 0 . z z ± ≠ ∈ Then, the following theorem, based on Proposition 3.1 and the ergodicity results of [15,29,30] that the Lebesgue measure λ on  is also ergodic with respect to the mappings ( 25) and ( 26), we obtain that any function 2 ( ) g L ∈  allows the direct sum orthogonal decomposition (22).…”
Section: Main Invariant Decomposition Results and Examplesmentioning
confidence: 91%
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“…for any 0 . z z ± ≠ ∈ Then, the following theorem, based on Proposition 3.1 and the ergodicity results of [15,29,30] that the Lebesgue measure λ on  is also ergodic with respect to the mappings ( 25) and ( 26), we obtain that any function 2 ( ) g L ∈  allows the direct sum orthogonal decomposition (22).…”
Section: Main Invariant Decomposition Results and Examplesmentioning
confidence: 91%
“…Proof. Proof easily follows from the ergodicity property of the Lebesgue measure λ on  stated in [29] and the α-invariance property of Remark 3.2. Consider now a so-called [31] internal function ( , ) : ω ω ± ± ∈  Taking into account now that the fixed points , ( , )…”
Section: Main Invariant Decomposition Results and Examplesmentioning
confidence: 99%
“…2 ((R m ) ⊗N ; C) is the corresponding symmetric ground-state wave function of the related quantum Hamiltonian system, satisfying the conditions ( 49) and (49), reduced on the invariant subspace Φ N . Moreover, the following general expressions hold: Ω(η) = 1 and for any ω ∈ L (µ)…”
Section: Non-relativistic Quantum Current Algebra and Its Cyclic Repr...mentioning
confidence: 99%
“…In particular, it was observed [25][26][27][28][29][30][31][32][33] that these structures are canonically related to each other. Mathematical properties, lying in a background of their analytical description, make it possible to study additional important parameters [34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50] of different hydrodynamic and magnetohydrodynamic systems, amongst which we will mention integral invariants, describing such internal fluid motion peculiarities as vortices, topological singularities [51] and other different instability states, strongly depending [52,53] on imposed isentropic fluid motion constraints. Being interested in their general properties and mathematical structures, responsible for their existence and behavior, we present a detailed enough differential geometrical approach to investigating thermodynamically quasi-stationary isentropic fluid motions, paying more attention to analytical argumentation of tricks and techniques used during the presentation.…”
Section: Diffeomorphism Group Structure and Functional Phase Space De...mentioning
confidence: 99%
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