Carlos F. Álvarez’s research while affiliated with University of Valparaíso and other places

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Publications (7)


Dynamical Properties for Composition Operators on H^{2}({\mathbb {C}}_{+})
  • Article

January 2025

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9 Reads

Boletim da Sociedade Brasileira de Matemática

Carlos F. Álvarez

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In this article, we investigate expansivity, Li–Yorke chaos and shadowing properties for composition operators Cϕf=fϕC_{\phi }f = f \circ \phi induced by affine self-maps ϕ\phi of the right half-plane C+{\mathbb {C}}_{+} on the Hardy–Hilbert space H2(C+)H^{2}(\mathbb {C_{+}}).


On the composition operator with variable integrability
  • Article
  • Full-text available

January 2025

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8 Reads

AIMS Mathematics

In this article, we considered a class of composition operators on Lebesgue spaces with variable exponents over metric measure spaces. Taking advantage of the compatibility between the metric-measurable structure and the regularity properties of the variable exponent, we provided necessary and sufficient conditions for this class of operators to be bounded and compact, respectively. In addition, we showed the usefulness of the variable change to study weak compactness properties in the framework of non-standard spaces.

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On Koopman operator with variable integrability

October 2024

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12 Reads

In this note, we consider a class of composition operators on Lebesgue spaces with variable exponents over metric measure spaces. Taking advantage of the compatibility between the metric-measurable structure and the regularity properties of the variable exponent, we provide necessary and sufficient conditions for this class of operators to be bounded and compact, respectively. In addition, we show the usefulness of the variable change to study weak compactness properties in the framework of non-standard spaces.


π-1(B(x,β))≃B(x,β)×π-1({x})\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\pi ^{-1}(B(x, \beta )) \simeq B(x, \beta ) \times \pi ^{-1}(\{x\})$$\end{document} represented for a two-dimensional case, in which we have dynamical coherence and the center leaves are well defined
The box V~(x~)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\tilde{V}(\tilde{x})$$\end{document} contained in the connected component of x~\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\tilde{x}$$\end{document} on π-1(B(x,β))\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\pi ^{-1}(B(x, \beta ))$$\end{document}, represented here for the two-dimensional case
The map g is constructed by perturbing B along the unstable (vertical) direction, maintaining the vertical foliation as a g-invariant foliation. We create on the unstable line of the fixed point p0=(0,0)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$p_0 = (0, 0)$$\end{document} two new fixed points in such way that it changes the stable index of p0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$p_0$$\end{document}, so that g is not uniformly hyperbolic
Equilibrium States for Partially Hyperbolic Maps with One-Dimensional Center

November 2023

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34 Reads

Journal of Statistical Physics

We prove the existence of equilibrium states for partially hyperbolic endomorphisms with one-dimensional center bundle. We also prove, regarding a class of potentials, the uniqueness of such measures for endomorphisms defined on the 2-torus that: have a linear model as a factor; and with the condition that this measure gives zero weight to the set where the conjugacy with the linear model fails to be invertible. In particular, we obtain the uniqueness of the measure of maximal entropy. For the n-torus, the uniqueness in the case with one-dimensional center holds for absolutely partially hyperbolic maps with additional hypotheses on the invariant leaves, namely, dynamical coherence and quasi-isometry. We provide an example satisfying these hypotheses.


Dynamical Properties for Composition Operators on $H^{2}(\mathbb{C}_{+})

June 2023

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89 Reads

Expansivity, Li-Yorke chaos and shadowing are popular and well-studied notions of dynamical systems. Several simple and useful characterizations of these notions within the setting of linear dynamics were obtained recently.Expansivity, Li-Yorke chaos and shadowing are popular and well-studied notions of dynamical systems. Several simple and useful characterizations of these notions within the setting of linear dynamics were obtained recently. In this paper, we characterize these three dynamical properties for composition operators Cϕf=fϕC_{\phi}f = f \circ \phi induced by affine self-maps ϕ\phi of the right half-plane C+\mathbb{C}_{+} on the Hardy-Hilbert space H2(C+)H^{2}(\mathbb{C_{+}}).


Existence and uniqueness of measures of maximal entropy for partially hyperbolic endomorphisms

July 2022

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6 Reads

We prove the existence of equilibrium states for partially hyperbolic endomorphisms with one-dimensional center bundle. We also prove, regarding a class of potentials, the uniqueness of such measures for endomorphisms defined on the 2-torus that: have a linear model as a factor; and with the condition that this measure gives zero weight to the set where the conjugacy with the linear model fails to be invertible. In particular, we obtain the uniqueness of the measure of maximal entropy. For the n-torus, the uniqueness in the case with one-dimensional center holds for absolutely partially hyperbolic maps with additional hypotheses on the invariant leaves, namely, dynamical coherence and quasi-isometry.