{"id":1068,"date":"2021-04-12T05:26:35","date_gmt":"2021-04-12T05:26:35","guid":{"rendered":"http:\/\/jangadadinamica.com\/?page_id=1068"},"modified":"2026-01-24T21:52:41","modified_gmt":"2026-01-24T21:52:41","slug":"articles","status":"publish","type":"page","link":"https:\/\/yurilima-math.com\/?page_id=1068","title":{"rendered":"Publications"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"1068\" class=\"elementor elementor-1068\" data-elementor-post-type=\"page\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-2402091b elementor-section-full_width elementor-section-height-default elementor-section-height-default\" data-id=\"2402091b\" data-element_type=\"section\" data-e-type=\"section\" data-settings=\"{&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-no\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-35ff605c\" data-id=\"35ff605c\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-inner-section elementor-element elementor-element-46c38faa elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"46c38faa\" data-element_type=\"section\" data-e-type=\"section\" data-settings=\"{&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-no\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-inner-column elementor-element elementor-element-3d4b90c4\" data-id=\"3d4b90c4\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-ec11118 elementor-widget elementor-widget-image\" data-id=\"ec11118\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img decoding=\"async\" src=\"https:\/\/yurilima-math.com\/wp-content\/uploads\/elementor\/thumbs\/articles-pxuq2aaczhbmg86nnr4ycheouhu589eup0w9bg37i0.png\" title=\"articles\" alt=\"articles\" loading=\"lazy\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-45b771d elementor-widget elementor-widget-spacer\" data-id=\"45b771d\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-815f0a2 elementor-widget elementor-widget-heading\" data-id=\"815f0a2\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-xl\">Publications<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-49f4f10 elementor-widget elementor-widget-spacer\" data-id=\"49f4f10\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-85717c3 elementor-widget elementor-widget-accordion\" data-id=\"85717c3\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"accordion.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-accordion\">\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1391\" class=\"elementor-tab-title\" data-tab=\"1\" role=\"button\" aria-controls=\"elementor-tab-content-1391\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">29. Superdiffusive central limit theorems for geodesic flows on nonpositively curved surfaces<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1391\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"1\" role=\"region\" aria-labelledby=\"elementor-tab-title-1391\"><p>With <a href=\"http:\/\/carlos.matheus.perso.math.cnrs.fr\/\">C. Matheus<\/a> and <a href=\"https:\/\/warwick.ac.uk\/fac\/sci\/maths\/people\/staff\/ian_melbourne\/\">I. Melbourne<\/a>.<\/p><p>Abstract: We prove a nonstandard central limit theorem and weak invariance principle, with superdiffusive normalisation <span class=\"katex-eq\" data-katex-display=\"false\">(t\\log t)^{1\/2}<\/span>, for geodesic flows on a class of nonpositively curved surfaces with flat cylinder. We also prove that correlations decay at rate <span class=\"katex-eq\" data-katex-display=\"false\">t^{-1}<\/span>. An important ingredient of the proof, which is of independent interest, is an improved results on the regularity of the stable\/unstable foliations induced by the Green bundles.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2512.11051\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1392\" class=\"elementor-tab-title\" data-tab=\"2\" role=\"button\" aria-controls=\"elementor-tab-content-1392\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">28. Uniqueness of the measure of maximal entropy for geodesic flows on surfaces<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1392\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"2\" role=\"region\" aria-labelledby=\"elementor-tab-title-1392\"><p>With <a href=\"https:\/\/sites.google.com\/mathematics.byu.edu\/davi-obata\/home\">D. Obata<\/a> and <a href=\"https:\/\/sites.google.com\/mat.ufc.br\/mpoletti\">M. Poletti<\/a>.<\/p><p>Abstract: We prove that if a geodesic flow on a closed orientable <span class=\"katex-eq\" data-katex-display=\"false\">C^\\infty<\/span> surface is transitive and has positive topological entropy, then it has a unique measure of maximal entropy. This covers all previous results of the literature on the uniqueness of the measure of maximal entropy in this context, as well as it applies to new examples such as the ones constructed by Donnay and Burns-Donnay. We also prove that, in the above context, there is at most one SRB measure.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2511.22022\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1393\" class=\"elementor-tab-title\" data-tab=\"3\" role=\"button\" aria-controls=\"elementor-tab-content-1393\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">27. Symbolic dynamics for non-uniformly hyperbolic flows in high dimension<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1393\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"3\" role=\"region\" aria-labelledby=\"elementor-tab-title-1393\"><p>With J.C. Mongez and J.P. Nascimento.<\/p><p>Abstract: We construct symbolic dynamics for flows with positive speed in any dimension: for each <span class=\"katex-eq\" data-katex-display=\"false\"> \\chi&gt;0<\/span>, we code a set that has full measure for every invariant probability measure which is <span class=\"katex-eq\" data-katex-display=\"false\">\\chi<\/span>&#8211;hyperbolic. In particular, the coded set contains all hyperbolic periodic orbits with Lyapunov exponents outside of <span class=\"katex-eq\" data-katex-display=\"false\">[-\\chi,\\chi]<\/span>. This extends the recent work of Buzzi, Crovisier, and Lima for three dimensional flows with positive speed. As an application, we code homoclinic classes of measures by suspensions of irreducible countable Markov shifts, and prove that each such class has at most one probability measure that maximizes the entropy.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2509.09050\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1394\" class=\"elementor-tab-title\" data-tab=\"4\" role=\"button\" aria-controls=\"elementor-tab-content-1394\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">26. Nonstandard functional central limit theorem for nonuniformly hyperbolic dynamical systems, including Bunimovich stadia<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1394\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"4\" role=\"region\" aria-labelledby=\"elementor-tab-title-1394\"><p>With <a href=\"http:\/\/carlos.matheus.perso.math.cnrs.fr\/\">C. Matheus<\/a> and <a href=\"https:\/\/warwick.ac.uk\/fac\/sci\/maths\/people\/staff\/ian_melbourne\/\">I. Melbourne<\/a>.<\/p><p>Abstract: We consider a class of nonuniformly hyperbolic dynamical systems with a first return time satisfying a central limit theorem (CLT) with nonstandard normalisation <span class=\"katex-eq\" data-katex-display=\"false\">(n\\log n)^{1\/2}<\/span>. For such systems (both maps and flows) we show that it automatically follows that the functional central limit theorem or weak invariance principle (WIP) with normalisation <span class=\"katex-eq\" data-katex-display=\"false\">(n\\log n)^{1\/2}<\/span> holds for H\u00f6lder observables. Our approach streamlines certain arguments in the literature. Applications include various examples from billiards, geodesic flows and intermittent dynamical systems. In this way, we unify existing results as well as obtaining new results. In particular, we deduce the WIP with nonstandard normalisation for Bunimovich stadia as an immediate consequence of the corresponding CLT proved by B\u00e1lint &amp; Gou\u00ebzel.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2507.03204\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1395\" class=\"elementor-tab-title\" data-tab=\"5\" role=\"button\" aria-controls=\"elementor-tab-content-1395\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">25. Equilibrium states by synchronization, symbolic extensions, and factors<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1395\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"5\" role=\"region\" aria-labelledby=\"elementor-tab-title-1395\"><p>With <a href=\"https:\/\/sites.google.com\/view\/gelfert\">Katrin Gelfert<\/a> and <a href=\"https:\/\/www2.im.uj.edu.pl\/DominikKwietniak\/\">Dominik Kwietniak<\/a>.<\/p><p>Abstract: We combine the two classical topological concepts, time-preserving topological factors and synchronizing time-changes of a continuous flow, and explore some of their thermodynamic consequences. Particular focus is put on equilibrium states and, in particular, measures of maximal entropy, with emphasis on geodesic flows on rank-one surfaces of nonpositive curvature and their time-preserving expansive topological factors for which we investigate the scaled geometric potentials.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2503.18193\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1396\" class=\"elementor-tab-title\" data-tab=\"6\" role=\"button\" aria-controls=\"elementor-tab-content-1396\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">24. Measures of maximal entropy for non-uniformly hyperbolic maps<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1396\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"6\" role=\"region\" aria-labelledby=\"elementor-tab-title-1396\"><p>With <a href=\"https:\/\/sites.google.com\/mathematics.byu.edu\/davi-obata\/home\">D. Obata<\/a> and <a href=\"https:\/\/sites.google.com\/mat.ufc.br\/mpoletti\">M. Poletti<\/a>.<\/p><p>J. Eur. Math. Soc. (2026), published online first. DOI: 10.4171\/JEMS\/1767<\/p><p>Abstract: For <span class=\"katex-eq\" data-katex-display=\"false\">C^{1+}<\/span> maps, possibly non-invertible and with singularities, we prove that each homoclinic class of an adapted hyperbolic measure carries at most one adapted hyperbolic measure of maximal entropy. We then apply this to study the finiteness\/uniqueness of such measures in several different settings: finite horizon dispersing billiards, codimension one partially hyperbolic endomorphisms with &#8220;large&#8221; entropy, robustly non-uniformly hyperbolic volume-preserving endomorphisms as in Andersson-Carrasco-Saghin, and strongly transitive non-uniformly expanding maps.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2405.04676\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1397\" class=\"elementor-tab-title\" data-tab=\"7\" role=\"button\" aria-controls=\"elementor-tab-content-1397\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">23. Symbolic dynamics for large non-uniformly hyperbolic sets of three dimensional flows<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1397\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"7\" role=\"region\" aria-labelledby=\"elementor-tab-title-1397\"><p>With <a href=\"https:\/\/www.imo.universite-paris-saclay.fr\/~jerome.buzzi\/\">J\u00e9r\u00f4me Buzzi<\/a> and <a href=\"https:\/\/www.imo.universite-paris-saclay.fr\/~sylvain.crovisier\/\">Sylvain Crovisier<\/a>.<\/p><p>Adv. Math. 479 (2025), Paper No. 110410.<\/p><p><span style=\"font-family: var( --e-global-typography-text-font-family ), Sans-serif; font-weight: var( --e-global-typography-text-font-weight ); background-color: var( --e-global-color-accent ); font-size: 1rem;\">Abstract:\u00a0<\/span><span style=\"background-color: var( --e-global-color-accent );\">We construct symbolic dynamics for three dimensional flows with positive speed. More precisely, for each <span class=\"katex-eq\" data-katex-display=\"false\"> \\chi&gt;0 <\/span>, we code a set of full measure for every invariant probability measure which is <span class=\"katex-eq\" data-katex-display=\"false\"> \\chi<\/span>&#8211;hyperbolic. These include all ergodic measures with entropy bigger than \u03c7 as well as all hyperbolic periodic orbits of saddle-type with Lyapunov exponent outside of <span class=\"katex-eq\" data-katex-display=\"false\"> [-\\chi,\\chi]<\/span>. This contrasts with a previous work of Lima &amp; Sarig which built a coding associated to a given invariant probability measure. As an application, we code homoclinic classes of measures by suspensions of irreducible countable Markov shifts.<\/span><\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2307.14319\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1398\" class=\"elementor-tab-title\" data-tab=\"8\" role=\"button\" aria-controls=\"elementor-tab-content-1398\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">22. P\u00f3lya urns on hypergraphs<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1398\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"8\" role=\"region\" aria-labelledby=\"elementor-tab-title-1398\"><p>With Pedro Alves and Matheus Barros.<\/p><p>Nonlinearity (2025), Volume 38, Number 7<\/p><p>Abstract: We study P\u00f3lya urns on hypergraphs and prove that, when the incidence matrix of the hypergraph is injective, there exists a point <span class=\"katex-eq\" data-katex-display=\"false\">v=v(H)<\/span> such that the random process converges to v almost surely. We also provide a partial result when the incidence matrix is not injective.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2310.00159\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-1399\" class=\"elementor-tab-title\" data-tab=\"9\" role=\"button\" aria-controls=\"elementor-tab-content-1399\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">21. Homoclinic classes of geodesic flows on rank 1 manifolds<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1399\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"9\" role=\"region\" aria-labelledby=\"elementor-tab-title-1399\"><p>With <a href=\"https:\/\/sites.google.com\/mat.ufc.br\/mpoletti\">Mauricio Poletti<\/a>.<\/p><p>Proc. Amer. Math. Soc. 153 (2025), no. 4, 1611\u20131620.<\/p><p>Abstract: We prove that the homoclinic class of every hyperbolic periodic orbit of a geodesic flow over a <span class=\"katex-eq\" data-katex-display=\"false\">C^\\infty<\/span> closed rank 1 Riemannian manifold equals the unit tangent bundle. As an application, we give a proof using symbolic dynamics of the theorem of Knieper on the uniqueness of the measure of maximal entropy and theorems of Burns et al on the uniqueness of equilibrium states.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2403.03759\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13910\" class=\"elementor-tab-title\" data-tab=\"10\" role=\"button\" aria-controls=\"elementor-tab-content-13910\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">20. Symbolic dynamics for nonuniformly hyperbolic maps with singularities in high dimension<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13910\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"10\" role=\"region\" aria-labelledby=\"elementor-tab-title-13910\"><p>With <a href=\"https:\/\/sigaa.ufma.br\/sigaa\/public\/docente\/portal.jsf?siape=3249334&amp;lc=en_US\">E. Araujo<\/a> and <a href=\"https:\/\/sites.google.com\/mat.ufc.br\/mpoletti\">M. Poletti<\/a>.<\/p><p>Memoirs of the American Mathematical Society 301 (2024), number 1511.<\/p><p>Abstract: We construct Markov partitions for non-invertible and\/or singular nonuniformly hyperbolic systems defined on higher dimensional Riemannian manifolds. The generality of the setup covers classical examples not treated so far, such as geodesic flows in closed manifolds, multidimensional billiard maps, and Viana maps, and includes all the recent results of the literature. We also provide a wealth of applications.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2010.11808\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13911\" class=\"elementor-tab-title\" data-tab=\"11\" role=\"button\" aria-controls=\"elementor-tab-content-13911\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">19. Polynomial decay of correlations for nonpositively curved surfaces<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13911\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"11\" role=\"region\" aria-labelledby=\"elementor-tab-title-13911\"><p>With <a href=\"http:\/\/carlos.matheus.perso.math.cnrs.fr\/\">C. Matheus<\/a> and <a href=\"https:\/\/warwick.ac.uk\/fac\/sci\/maths\/people\/staff\/ian_melbourne\/\">I. Melbourne<\/a>.<\/p><p>Transactions of the AMS 377 (2024), no. 9, 6043\u20136095.<\/p><p>Abstract: We prove polynomial decay of correlations for geodesic flows on a class of nonpositively curved surfaces where zero curvature only occurs along one closed geodesic. We also prove that various statistical limit laws, including the central limit theorem, are satisfied by this class of geodesic flows.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2107.11805\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13912\" class=\"elementor-tab-title\" data-tab=\"12\" role=\"button\" aria-controls=\"elementor-tab-content-13912\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">18. Lyapunov exponents and nonadapted measures for dispersing billiards<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13912\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"12\" role=\"region\" aria-labelledby=\"elementor-tab-title-13912\"><p>With <a href=\"https:\/\/www.math.uh.edu\/~climenha\/\">Vaughn Climenhaga<\/a>, <a href=\"http:\/\/www.faculty.fairfield.edu\/mdemers\/\">Mark Demers<\/a> and <a href=\"https:\/\/people.math.umass.edu\/~hongkun\/\">Hongkun Zhang<\/a><span style=\"background-color: var( --e-global-color-accent );\">.<\/span><\/p><p><span style=\"background-color: var( --e-global-color-accent );\">Commun. Math. Phys. 405, 24 (2024).<br \/><\/span><\/p><p><span style=\"font-family: var( --e-global-typography-text-font-family ), Sans-serif; font-weight: var( --e-global-typography-text-font-weight ); background-color: var( --e-global-color-accent ); font-size: 1rem;\">Abstract: For hyperbolic systems with singularities, such as dispersing billiards, Pesin theory as developed by Katok and Strelcyn applies to measures that are &#8220;adapted&#8221; in the sense that they do not give too much weight to neighborhoods of the singularity set. The zero-entropy measures supported on grazing periodic orbits are nonadapted, but it has been an open question whether there are nonadapted measures with positive entropy. We construct such measures for any dispersing billiard with a periodic orbit having a single grazing collision; we then use our construction to show that the thermodynamic formalism for such billiards has a phase transition even when one restricts attention to adapted or to positive entropy measures.<\/span><\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2308.08042\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13913\" class=\"elementor-tab-title\" data-tab=\"13\" role=\"button\" aria-controls=\"elementor-tab-content-13913\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">17. Examples of <span class=\"katex-eq\" data-katex-display=\"false\"> d<\/span>\u2212sets with irregular projection of Hausdorff measures<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13913\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"13\" role=\"region\" aria-labelledby=\"elementor-tab-title-13913\"><p>With <a href=\"https:\/\/w3.impa.br\/~gugu\/\">C. G. Moreira<\/a>.<\/p><p><span style=\"background-color: var( --e-global-color-accent );\">Bull. Braz. Math. Soc. (N.S.) 54 (2023), no. 2, Paper No. 28, 4 pp.<\/span><\/p><p>Abstract: Given positive integers <span class=\"katex-eq\" data-katex-display=\"false\"> \\ell&lt;n <\/span> and a real <span class=\"katex-eq\" data-katex-display=\"false\"> d\\in (\\ell,n) <\/span>, we construct sets <span class=\"katex-eq\" data-katex-display=\"false\"> K\\subset R^n <\/span> with positive and finite Hausdorff <span class=\"katex-eq\" data-katex-display=\"false\"> d<\/span>\u2212measure such that the Radon-Nikodym derivative associated to all projections on <span class=\"katex-eq\" data-katex-display=\"false\"> \\ell <\/span>\u2212dimensional planes is not an <span class=\"katex-eq\" data-katex-display=\"false\"> L^p <\/span> function, for all <span class=\"katex-eq\" data-katex-display=\"false\"> p&gt;1<\/span>.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/2301.07744\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13914\" class=\"elementor-tab-title\" data-tab=\"14\" role=\"button\" aria-controls=\"elementor-tab-content-13914\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">16. Symbolic dynamics for nonuniformly hyperbolic systems<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13914\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"14\" role=\"region\" aria-labelledby=\"elementor-tab-title-13914\"><p>Ergodic Theory Dynam. Systems <strong>41<\/strong> (2021), no. 9, 2591-2658.<\/p><p>Abstract: This survey describes the recent advances in the construction of Markov partitions for non-uniformly hyperbolic systems. One important feature of this development comes from a finer theory of non-uniformly hyperbolic systems, which we also describe. The Markov partition defines a symbolic extension that is finite-to-one and onto a non-uniformly hyperbolic locus, and this provides dynamical and statistical consequences such as estimates on the number of closed orbits and properties of equilibrium measures. The class of systems includes diffeomorphisms, flows, and maps with singularities.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/1910.11371\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13915\" class=\"elementor-tab-title\" data-tab=\"15\" role=\"button\" aria-controls=\"elementor-tab-content-13915\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">15. Simplicity of Lyapunov spectrum for linear cocycles over non-uniformly hyperbolic systems<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13915\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"15\" role=\"region\" aria-labelledby=\"elementor-tab-title-13915\"><p>With <a href=\"http:\/\/www.mat.ufrgs.br\/~backes\/\">L. Backes<\/a>, <a href=\"https:\/\/sites.google.com\/mat.ufc.br\/mpoletti\">M. Poletti<\/a>, and <a href=\"https:\/\/sites.google.com\/view\/paulovarandas\/\">P. Varandas<\/a>.<\/p><p>Ergodic Theory Dynam. Systems <strong>40<\/strong> (2020), no. 11, 2947-2969.<\/p><p>Abstract: We prove that generic fiber-bunched and H\u00f6lder continuous linear cocycles over a non-uniformly hyperbolic system endowed with a <span class=\"katex-eq\" data-katex-display=\"false\">u<\/span>-Gibbs measure have simple Lyapunov spectrum. This gives an affirmative answer to a conjecture proposed by Viana in the context of fiber-bunched linear cocycles.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/1612.05056\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13916\" class=\"elementor-tab-title\" data-tab=\"16\" role=\"button\" aria-controls=\"elementor-tab-content-13916\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">14. Symbolic dynamics for one dimensional maps with nonuniform expansion<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13916\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"16\" role=\"region\" aria-labelledby=\"elementor-tab-title-13916\"><p>Ann. Inst. H. Poincar\u00e9 C Anal. Non Lin\u00e9aire <strong>37<\/strong> (2020), no. 3, 727-755.<\/p><p class=\"p1\">Abstract: Given a piecewise <span class=\"katex-eq\" data-katex-display=\"false\">C^{1+\\beta}<\/span> map of the interval, possibly with critical points and discontinuities, we construct a symbolic model for invariant probability measures with nonuniform expansion that do not approach the critical points and discontinuities exponentially fast almost surely. More specifically, for each <span class=\"katex-eq\" data-katex-display=\"false\">\\chi&gt;0<\/span> we construct a finite-to-one H\u00f6lder continuous map from a countable topological Markov shift to the natural extension of the interval map, that codes the lifts of all invariant probability measures as above with Lyapunov exponent greater than <span class=\"katex-eq\" data-katex-display=\"false\">\\chi<\/span> almost everywhere.<\/p><p class=\"p1\"><a href=\"https:\/\/arxiv.org\/abs\/1801.03359\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13917\" class=\"elementor-tab-title\" data-tab=\"17\" role=\"button\" aria-controls=\"elementor-tab-content-13917\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">13. Symbolic dynamics for three dimensional flows with positive topological entropy<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13917\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"17\" role=\"region\" aria-labelledby=\"elementor-tab-title-13917\"><p>With <a href=\"https:\/\/www.weizmann.ac.il\/math\/sarigo\/\">O. Sarig<\/a>.<\/p><p>J. Eur. Math. Soc. (JEMS) <strong>21<\/strong> (2019), no. 1, 199-256.<\/p><p class=\"p1\">Abstract: We construct symbolic dynamics on sets of full measure (with respect to an ergodic measure of positive entropy) for <span class=\"katex-eq\" data-katex-display=\"false\">C^{1+\\epsilon}<\/span> flows on closed smooth three-dimensional manifolds. One consequence is that the geodesic flow on the unit tangent bundle of a closed <span class=\"katex-eq\" data-katex-display=\"false\">C^\\infty<\/span>surface has at least const<span class=\"katex-eq\" data-katex-display=\"false\">\\times e^{hT}\/T<\/span> simple closed orbits of period less than <span class=\"katex-eq\" data-katex-display=\"false\">T<\/span>, whenever the topological entropy <span class=\"math math-inline\"><span class=\"katex css-afhwjo\"><span class=\"katex-mathml\"><span class=\"katex-eq\" data-katex-display=\"false\">h<\/span><\/span><\/span><\/span> is positive &#8211; and without further assumptions on the curvature.<\/p><p class=\"p1\"><a href=\"https:\/\/arxiv.org\/abs\/1408.3427\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13918\" class=\"elementor-tab-title\" data-tab=\"18\" role=\"button\" aria-controls=\"elementor-tab-content-13918\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">12. Symbolic dynamics for non-uniformly hyperbolic surface maps with discontinuities<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13918\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"18\" role=\"region\" aria-labelledby=\"elementor-tab-title-13918\"><p>With <a href=\"http:\/\/carlos.matheus.perso.math.cnrs.fr\/\">C. Matheus<\/a>.<\/p><p>Ann. Sci. \u00c9c. Norm. Sup\u00e9r. (4) <strong>51<\/strong> (2018), no. 1, 1-38.<\/p><p class=\"p1\">Abstract: This work constructs symbolic dynamics for non-uniformly hyperbolic surface maps with a set of discontinuities <span class=\"katex-eq\" data-katex-display=\"false\">\\mathcal D<\/span>. We allow the derivative of points nearby <span class=\"katex-eq\" data-katex-display=\"false\">\\mathcal D<\/span> to be unbounded, of the order of a negative power of the distance to <span class=\"katex-eq\" data-katex-display=\"false\">\\mathcal D<\/span>. Under natural geometrical assumptions on the underlying space <span class=\"katex-eq\" data-katex-display=\"false\">M<\/span>, we code a set of non-uniformly hyperbolic orbits that do not converge exponentially fast to <span class=\"katex-eq\" data-katex-display=\"false\">\\mathcal D<\/span>. The results apply to non-uniformly hyperbolic planar billiards, e.g. Bunimovich billiards.<\/p><p class=\"p1\"><a href=\"https:\/\/arxiv.org\/abs\/1606.05863\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13919\" class=\"elementor-tab-title\" data-tab=\"19\" role=\"button\" aria-controls=\"elementor-tab-content-13919\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">11. Ergodic properties of skew products in infinite measure<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13919\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"19\" role=\"region\" aria-labelledby=\"elementor-tab-title-13919\"><p>With <a href=\"https:\/\/www.somos.unifesp.br\/professor\/patricia-romano-cirilo\">P. Cirilo<\/a> and <a href=\"https:\/\/www.gc.cuny.edu\/people\/enrique-pujals\">E. Pujals<\/a>.<\/p><p>Israel J. Math. <strong>214<\/strong> (2016), no. 1, 43-66.<\/p><p class=\"p1\">Abstract: Let <span class=\"katex-eq\" data-katex-display=\"false\">(\\Omega,\\mu)<\/span> be a shift of finite type with a Markov probability, and <span class=\"katex-eq\" data-katex-display=\"false\">(Y,\\nu)<\/span> a non-atomic standard measure space. For each symbol <span class=\"katex-eq\" data-katex-display=\"false\">i<\/span> of the symbolic space, let <span class=\"katex-eq\" data-katex-display=\"false\">\\Phi_i<\/span> be a non-singular automorphism of <span class=\"katex-eq\" data-katex-display=\"false\">(Y,\\nu)<\/span>. We study skew products of the form <span class=\"katex-eq\" data-katex-display=\"false\">(\\omega,y)\\mapsto (\\sigma\\omega,\\Phi_{\\omega_0}(y))<\/span>, where <span class=\"katex-eq\" data-katex-display=\"false\">\\sigma<\/span> is the shift map on <span class=\"katex-eq\" data-katex-display=\"false\">(\\Omega,\\mu)<\/span>. We prove that, when the skew product is recurrent, it is ergodic if and only if the <span class=\"katex-eq\" data-katex-display=\"false\">\\Phi_i<\/span>&#8216;s have no common non-trivial invariant set.<\/p><p>In the second part we study the skew product when <span class=\"katex-eq\" data-katex-display=\"false\">\\Omega=\\{0,1\\}^{\\mathbb Z}<\/span>, <span class=\"katex-eq\" data-katex-display=\"false\">\\mu<\/span> is a Bernoulli measure, and <span class=\"katex-eq\" data-katex-display=\"false\">\\Phi_0,\\Phi_1<\/span> are <span class=\"katex-eq\" data-katex-display=\"false\">\\mathbb R<\/span>-extensions of a same uniquely ergodic probability-preserving automorphism. We prove that, for a large class of roof functions, the skew product is rationally ergodic with return sequence asymptotic to <span class=\"katex-eq\" data-katex-display=\"false\">\\sqrt{n}<\/span>, and its trajectories satisfy the central, functional central and local limit theorem.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/1210.4382\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13920\" class=\"elementor-tab-title\" data-tab=\"20\" role=\"button\" aria-controls=\"elementor-tab-content-13920\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">10. Ergodic properties of equilibrium measures for smooth three dimensional flows<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13920\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"20\" role=\"region\" aria-labelledby=\"elementor-tab-title-13920\"><p>With <a href=\"https:\/\/en.wikipedia.org\/wiki\/Fran%C3%A7ois_Ledrappier\">F. Ledrappier<\/a> and <a href=\"https:\/\/www.weizmann.ac.il\/math\/sarigo\/\">O. Sarig<\/a>.<\/p><p>Comment. Math. Helv. <strong>91<\/strong> (2016), no. 1, 65-106.<\/p><p class=\"p1\">Abstract: Let <span class=\"katex-eq\" data-katex-display=\"false\">\\{T^t\\}<\/span>\u00a0be a smooth flow with positive speed and positive topological entropy on a compact smooth three dimensional manifold, and let <span class=\"math math-inline\"><span class=\"katex css-afhwjo\"><span class=\"katex-mathml\">\u03bc\\mu<\/span><span class=\"katex-html\" aria-hidden=\"true\"><span class=\"base\"><span class=\"mord mathnormal\">\u03bc<\/span><\/span><\/span><\/span><\/span> be an ergodic measure of maximal entropy. We show that either <span class=\"katex-eq\" data-katex-display=\"false\">\\{T^t\\}<\/span> is Bernoulli, or <span class=\"katex-eq\" data-katex-display=\"false\">\\{T^t\\}<\/span>\u00a0is isomorphic to the product of a Bernoulli flow and a rotational flow. Applications are given to Reeb flows.<\/p><p class=\"p1\"><a href=\"https:\/\/arxiv.org\/abs\/1504.00048\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13921\" class=\"elementor-tab-title\" data-tab=\"21\" role=\"button\" aria-controls=\"elementor-tab-content-13921\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">9. Graph-based P\u00f3lya's urn: completion of the linear case<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13921\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"21\" role=\"region\" aria-labelledby=\"elementor-tab-title-13921\"><p>Stoch. Dyn. <strong>16<\/strong> (2016), no. 2, 1660007, 13 pp.<\/p><p class=\"p1\">Abstract: Given a finite connected graph <span class=\"katex-eq\" data-katex-display=\"false\">G<\/span>, place a bin at each vertex. Two bins are called a pair if they share an edge of <span class=\"katex-eq\" data-katex-display=\"false\">G<\/span>. At discrete times, a ball is added to each pair of bins. In a pair of bins, one of the bins gets the ball with probability proportional to its current number of balls. This model was introduced by Benaim, Benjamini, Chen, and Lima. When <span class=\"katex-eq\" data-katex-display=\"false\">G<\/span> is not balanced bipartite, Chen and Lucas proved that the proportion of balls in the bins converges to a point <span class=\"katex-eq\" data-katex-display=\"false\">w(G)<\/span> almost surely.<\/p><p>We prove almost sure convergence for balanced bipartite graphs: the possible limit is either a single point <span class=\"katex-eq\" data-katex-display=\"false\">w(G)<\/span> or a closed interval <span class=\"katex-eq\" data-katex-display=\"false\">\\mathcal J(G)<\/span>.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/1409.7826\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13922\" class=\"elementor-tab-title\" data-tab=\"22\" role=\"button\" aria-controls=\"elementor-tab-content-13922\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">8. A generalized P\u00f3lya's urn with graph based interactions<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13922\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"22\" role=\"region\" aria-labelledby=\"elementor-tab-title-13922\"><p>With <a href=\"http:\/\/members.unine.ch\/michel.benaim\/perso\/benaim.html\">M. Bena\u00efm<\/a>, <a href=\"https:\/\/www.wisdom.weizmann.ac.il\/~itai\/\">I. Benjamini<\/a>, and <a href=\"https:\/\/www.junchenphd.com\/\">J. Chen<\/a>.\u00a0<\/p><p>Random Structures Algorithms <strong>46<\/strong> (2015), no. 4, 614-634.<\/p><p class=\"p1\">Abstract: Given a finite connected graph <span class=\"katex-eq\" data-katex-display=\"false\">G<\/span>, place a bin at each vertex. Two bins are called a pair if they share an edge of <span class=\"katex-eq\" data-katex-display=\"false\">G<\/span>. At discrete times, a ball is added to each pair of bins. In a pair of bins, one of the bins gets the ball with probability proportional to its current number of balls raised by some fixed power <span class=\"katex-eq\" data-katex-display=\"false\">\\alpha&gt;0<\/span>. We characterize the limiting behavior of the proportion of balls in the bins.<\/p><p>The proof uses a dynamical approach to relate the proportion of balls to a vector field. Our main result is that the limit set of the proportion of balls is contained in the equilibria set of the vector field. We also prove that if <span class=\"katex-eq\" data-katex-display=\"false\">\\alpha&lt;1<\/span> then there is a single point <span class=\"katex-eq\" data-katex-display=\"false\">v=v(G,\\alpha)<\/span> with non-zero entries such that the proportion converges to <span class=\"katex-eq\" data-katex-display=\"false\">v<\/span> almost surely.<\/p><p>A special case is when <span class=\"katex-eq\" data-katex-display=\"false\">G<\/span> is regular and <span class=\"katex-eq\" data-katex-display=\"false\">\\alpha\\leq 1<\/span>. We show e.g. that if <span class=\"katex-eq\" data-katex-display=\"false\">G<\/span> is non-bipartite then the proportion of balls in the bins converges to the uniform measure almost surely.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/1211.1247\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13923\" class=\"elementor-tab-title\" data-tab=\"23\" role=\"button\" aria-controls=\"elementor-tab-content-13923\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">7. Annihilation and coalescence on binary trees<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13923\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"23\" role=\"region\" aria-labelledby=\"elementor-tab-title-13923\"><p class=\"p1\">With <a href=\"https:\/\/www.wisdom.weizmann.ac.il\/~itai\/\">I. Benjamini<\/a>.<\/p><p class=\"p1\">Stoch. Dyn. <strong>14<\/strong> (2014), no. 3, 1350023, 11 pp.<\/p><p class=\"p1\">Abstract: An infection spreads in a binary tree <span class=\"katex-eq\" data-katex-display=\"false\">\\mathcal T_n<\/span> of height <span class=\"katex-eq\" data-katex-display=\"false\">n<\/span> as follows: initially, each leaf is either infected by one of <span class=\"katex-eq\" data-katex-display=\"false\">k<\/span> states or it is not infected at all. The infection state of each leaf is independently distributed according to a probability vector <span class=\"katex-eq\" data-katex-display=\"false\">{\\bf p}=({\\bf p}_1,\\ldots,{\\bf p}_{k+1})<\/span>. The remaining nodes become infected or not via annihilation and coalescence: nodes whose two children have the same state (infected or not) are infected (or not) by this state; nodes whose two children have different states are not infected; nodes such that only one of the children is infected are infected by this state. In this paper we characterize, for every <span class=\"katex-eq\" data-katex-display=\"false\">{\\bf p}<\/span>, the limiting distribution at the root node of <span class=\"katex-eq\" data-katex-display=\"false\">\\mathcal T_n<\/span> as <span class=\"katex-eq\" data-katex-display=\"false\">n<\/span>\u00a0 goes to infinity.<\/p><div class=\"abstractSection abstractInFull\"><p>We also consider a variant of the model when <span class=\"katex-eq\" data-katex-display=\"false\">k=2<\/span> and a mutation can happen, with a fixed probability <span class=\"katex-eq\" data-katex-display=\"false\">q<\/span>, at each infection step. We characterize, in terms of <span class=\"katex-eq\" data-katex-display=\"false\">{\\bf p}<\/span> and <span class=\"katex-eq\" data-katex-display=\"false\">q<\/span>, the limiting distribution at the root node of <span class=\"katex-eq\" data-katex-display=\"false\">\\mathcal T_n<\/span> as <span class=\"katex-eq\" data-katex-display=\"false\">n<\/span> goes to infinity.<\/p><p>The distribution at the root node is driven by a dynamical system, and the proofs rely on the analysis of this dynamics.<\/p><p><a href=\"https:\/\/arxiv.org\/abs\/1305.2610\">Arxiv<\/a><\/p><\/div><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13924\" class=\"elementor-tab-title\" data-tab=\"24\" role=\"button\" aria-controls=\"elementor-tab-content-13924\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">6. An Abramov formula for stationary spaces of discrete groups<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13924\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"24\" role=\"region\" aria-labelledby=\"elementor-tab-title-13924\"><p class=\"p1\">With <a href=\"https:\/\/www.math.bgu.ac.il\/~hartmany\/\">Y. Hartman<\/a> and <a href=\"http:\/\/tamuz.caltech.edu\/\">O. Tamuz<\/a>.<\/p><p>Ergodic Theory Dynam. Systems <strong>34<\/strong> (2014), no. 3, 837\u2013853<\/p><p class=\"p1\">Abstract: Let <span class=\"katex-eq\" data-katex-display=\"false\">(G,\\mu)<\/span> be a discrete group equipped with a generating probability measure, and let <span class=\"katex-eq\" data-katex-display=\"false\">\\Gamma<\/span> be a finite index subgroup of <span class=\"katex-eq\" data-katex-display=\"false\">G<\/span>. A <span class=\"katex-eq\" data-katex-display=\"false\">\\mu<\/span>-random walk on <span class=\"katex-eq\" data-katex-display=\"false\">G<\/span>, starting from the identity, returns to <span class=\"katex-eq\" data-katex-display=\"false\">\\Gamma<\/span> with probability one. Let <span class=\"inlineFormula\"><span class=\"alternatives\"><span class=\"katex-eq\" data-katex-display=\"false\">\\theta<\/span><\/span><\/span> be the hitting measure, or the distribution of the position in which the random walk first hits <span class=\"inlineFormula\"><span class=\"alternatives\"><span class=\"katex-eq\" data-katex-display=\"false\">\\Gamma<\/span><\/span><\/span>. We prove that the Furstenberg entropy of a <span class=\"katex-eq\" data-katex-display=\"false\">(G,\\mu)<\/span>-stationary space, with respect to the action of <span class=\"katex-eq\" data-katex-display=\"false\">(\\Gamma,\\theta)<\/span>, is equal to the Furstenberg entropy with respect to the action of <span class=\"katex-eq\" data-katex-display=\"false\">(G,\\mu)<\/span>, times the index of <span class=\"inlineFormula\"><span class=\"alternatives\"><span class=\"katex-eq\" data-katex-display=\"false\">\\Gamma<\/span><\/span><\/span> in <span class=\"inlineFormula\"><span class=\"alternatives\"><span class=\"katex-eq\" data-katex-display=\"false\">G<\/span><\/span><\/span>. The index is shown to be equal to the expected return time to <span class=\"katex-eq\" data-katex-display=\"false\">\\Gamma<\/span>. As a corollary, when applied to the Furstenberg-Poisson boundary of <span class=\"katex-eq\" data-katex-display=\"false\">(G,\\mu)<\/span>, we prove that the random walk entropy of <span class=\"katex-eq\" data-katex-display=\"false\">(\\Gamma,\\theta)<\/span> is equal to the random walk entropy of <span class=\"inlineFormula\"><span class=\"alternatives\"><span class=\"katex-eq\" data-katex-display=\"false\">(G,\\mu)<\/span><\/span><\/span>, times the index of <span class=\"inlineFormula\"><span class=\"alternatives\"><span class=\"katex-eq\" data-katex-display=\"false\">\\Gamma<\/span><\/span><\/span> in <span class=\"inlineFormula\"><span class=\"alternatives\"><span class=\"katex-eq\" data-katex-display=\"false\">G<\/span>.<\/span><\/span><\/p><p class=\"p1\"><span class=\"inlineFormula\"><span class=\"alternatives\"><a href=\"https:\/\/arxiv.org\/abs\/1204.5414\">Arxiv<\/a><\/span><\/span><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13925\" class=\"elementor-tab-title\" data-tab=\"25\" role=\"button\" aria-controls=\"elementor-tab-content-13925\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">5. Law of large numbers for certain cylinder flows<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13925\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"25\" role=\"region\" aria-labelledby=\"elementor-tab-title-13925\"><p class=\"p1\">With <a href=\"https:\/\/www.somos.unifesp.br\/professor\/patricia-romano-cirilo\">P. Cirilo<\/a> and <a href=\"https:\/\/www.gc.cuny.edu\/people\/enrique-pujals\">E. Pujals<\/a>.<\/p><p>Ergodic Theory Dynam. Systems <strong>34<\/strong> (2014), no. 3, 801\u2013825<\/p><p class=\"p1\">Abstract: We construct new examples of cylinder flows, given by skew product extensions of irrational rotations on the circle, that are ergodic and rationally ergodic along a subsequence of iterates. In particular, they exhibit a law of large numbers. This is accomplished by explicitly calculating, for a subsequence of iterates, the number of visits to zero, and it is shown that such number has a Gaussian distribution.<\/p><p class=\"p1\"><a href=\"https:\/\/arxiv.org\/abs\/1108.3519\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13926\" class=\"elementor-tab-title\" data-tab=\"26\" role=\"button\" aria-controls=\"elementor-tab-content-13926\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">4. A Marstrand theorem for subsets of integers<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13926\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"26\" role=\"region\" aria-labelledby=\"elementor-tab-title-13926\"><p style=\"color: #000000;\">With <a href=\"https:\/\/w3.impa.br\/~gugu\/\">C. G. Moreira<\/a>.<\/p><p style=\"color: #000000;\">Combin. Probab. Comput. <span style=\"font-weight: bolder;\">23<\/span> (2014), no. 1, 116-134.<\/p><p style=\"color: #000000;\">Abstract: We propose a counting dimension for subsets of <span class=\"katex-eq\" data-katex-display=\"false\">\\mathbb Z<\/span> and prove that, under certain conditions on <span class=\"katex-eq\" data-katex-display=\"false\">E,F\\subset\\mathbb Z<\/span>, for Lebesgue almost every <span class=\"katex-eq\" data-katex-display=\"false\">\\lambda\\in\\mathbb R<\/span> the counting dimension of <span class=\"katex-eq\" data-katex-display=\"false\">E+\\lfloor \\lambda F\\rfloor<\/span> is at least the minimum between 1 and the sum of the counting dimensions of <span class=\"katex-eq\" data-katex-display=\"false\">E<\/span> and <span class=\"katex-eq\" data-katex-display=\"false\">F<\/span>. Furthermore, if the sum of the counting dimensions of <span class=\"katex-eq\" data-katex-display=\"false\">E<\/span> and <span class=\"katex-eq\" data-katex-display=\"false\">F<\/span> is larger than 1, then <span class=\"katex-eq\" data-katex-display=\"false\">E+\\lfloor \\lambda F\\rfloor<\/span> has positive upper Banach density for Lebesgue almost every <span class=\"katex-eq\" data-katex-display=\"false\">\\lambda\\in\\mathbb R<\/span>. The result has direct consequences when <span class=\"katex-eq\" data-katex-display=\"false\">E,F<\/span> are arithmetic sets, e.g., the integer values of a polynomial with integer coefficients.<\/p><p style=\"color: #000000;\"><a href=\"https:\/\/arxiv.org\/abs\/1011.0672\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13927\" class=\"elementor-tab-title\" data-tab=\"27\" role=\"button\" aria-controls=\"elementor-tab-content-13927\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">3. <span class=\"katex-eq\" data-katex-display=\"false\"> \\mathbb Z^d<\/span>-actions with prescribed topological and ergodic properties<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13927\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"27\" role=\"region\" aria-labelledby=\"elementor-tab-title-13927\"><p class=\"p1\" style=\"color: #000000;\">Ergodic Theory Dynam. Systems\u00a0 <strong>32<\/strong> (2012), no. 1, 191-209.<\/p><p class=\"p1\" style=\"color: #000000;\">Abstract: We extend constructions of Hahn and Katznelson [On the entropy of uniquely ergodic transformations. Trans. Amer. Math. Soc.126 (1967), 335\u2013360] and Pavlov [Some counterexamples in topological dynamics. Ergod. Th. &amp; Dynam. Sys.28 (2008), 1291\u20131322] to <span class=\"katex-eq\" data-katex-display=\"false\"> \\mathbb Z^d<\/span>-actions on symbolic dynamical spaces with prescribed topological and ergodic properties. More specifically, we describe a method to build <span class=\"katex-eq\" data-katex-display=\"false\"> \\mathbb Z^d<\/span>-actions which are (totally) minimal, (totally) strictly ergodic and have positive topological entropy.<\/p><p class=\"p1\" style=\"color: #000000;\"><a href=\"https:\/\/arxiv.org\/abs\/0912.2107\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13928\" class=\"elementor-tab-title\" data-tab=\"28\" role=\"button\" aria-controls=\"elementor-tab-content-13928\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">2. Yet another proof of Marstrand's theorem<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13928\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"28\" role=\"region\" aria-labelledby=\"elementor-tab-title-13928\"><p class=\"p1\" style=\"color: #000000;\">With <a href=\"https:\/\/w3.impa.br\/~gugu\/\">C. G. Moreira<\/a>.<\/p><p class=\"p1\" style=\"color: #000000;\">Bull. Braz. Math. Soc. <strong>42<\/strong> (2011), no. 2, 331-345.<\/p><p class=\"p1\" style=\"color: #000000;\">Abstract: In a paper from 1954 Marstrand proved that if\u00a0 <span class=\"katex-eq\" data-katex-display=\"false\"> K\\subset\\mathbb R^2 <\/span> is a Borel set with\u00a0 Hausdorff dimension greater than 1, then its one-dimensional projection has a positive Lebesgue measure for almost all directions. In this article, we give a combinatorial proof of this theorem, extending the techniques developed in our previous paper.<\/p><p class=\"p1\" style=\"color: #000000;\"><a href=\"https:\/\/arxiv.org\/abs\/1101.3252\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-accordion-item\">\n\t\t\t\t\t<div id=\"elementor-tab-title-13929\" class=\"elementor-tab-title\" data-tab=\"29\" role=\"button\" aria-controls=\"elementor-tab-content-13929\" aria-expanded=\"false\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon elementor-accordion-icon-right\" aria-hidden=\"true\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-closed\"><i class=\"fas fa-plus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t<span class=\"elementor-accordion-icon-opened\"><i class=\"fas fa-minus\"><\/i><\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"elementor-accordion-title\" tabindex=\"0\">1. A combinatorial proof of Marstrand's theorem for products of regular Cantor sets<\/a>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-13929\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"29\" role=\"region\" aria-labelledby=\"elementor-tab-title-13929\"><p class=\"p1\" style=\"color: #000000;\">With <a href=\"https:\/\/w3.impa.br\/~gugu\/\">C. G. Moreira<\/a>.<\/p><p class=\"p1\" style=\"color: #000000;\">Expo. Math.\u00a0<span style=\"font-weight: bolder;\">29<\/span>\u00a0(2011), no. 2, 231-239.<\/p><p class=\"p1\" style=\"color: #000000;\">Abstract: In a paper from 1954 Marstrand proved that if\u00a0 <span class=\"katex-eq\" data-katex-display=\"false\"> K\\subset\\mathbb R^2 <\/span> has a Hausdorff dimension greater than 1, then its one-dimensional projection has a positive Lebesgue measure for almost all directions. In this article, we give a combinatorial proof of this theorem when <span class=\"katex-eq\" data-katex-display=\"false\"> K <\/span> is the product of regular Cantor sets of class <span class=\"katex-eq\" data-katex-display=\"false\"> C^{1+\\alpha},\\alpha&gt;0<\/span>, for which the sum of their Hausdorff dimension is greater than 1.<\/p><p class=\"p1\" style=\"color: #000000;\"><a href=\"https:\/\/arxiv.org\/abs\/0911.1191\">Arxiv<\/a><\/p><\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-aa95984 elementor-widget elementor-widget-spacer\" data-id=\"aa95984\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<div class=\"elementor-element elementor-element-4049dbbc elementor-widget elementor-widget-google_maps\" data-id=\"4049dbbc\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"google_maps.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-custom-embed\">\n\t\t\t<iframe loading=\"lazy\"\n\t\t\t\t\tsrc=\"https:\/\/maps.google.com\/maps?q=Instituto%20de%20Matem%C3%A1tica%20e%20Estat%C3%ADstica&#038;t=m&#038;z=15&#038;output=embed&#038;iwloc=near\"\n\t\t\t\t\ttitle=\"Instituto de Matem\u00e1tica e Estat\u00edstica\"\n\t\t\t\t\taria-label=\"Instituto de Matem\u00e1tica e Estat\u00edstica\"\n\t\t\t><\/iframe>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<section class=\"elementor-section elementor-inner-section elementor-element elementor-element-98da4a6 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"98da4a6\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-inner-column elementor-element elementor-element-66c8311\" data-id=\"66c8311\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap\">\n\t\t\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-inner-column elementor-element elementor-element-dea9224\" data-id=\"dea9224\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-59a02ba1 elementor-shape-rounded elementor-grid-0 e-grid-align-center elementor-widget elementor-widget-social-icons\" data-id=\"59a02ba1\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"social-icons.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-social-icons-wrapper elementor-grid\" role=\"list\">\n\t\t\t\t\t\t\t<span class=\"elementor-grid-item\" role=\"listitem\">\n\t\t\t\t\t<a class=\"elementor-icon elementor-social-icon elementor-social-icon-instagram elementor-animation-grow elementor-repeater-item-d9a9500\" href=\"https:\/\/www.instagram.com\/jangadadinamica\/\" target=\"_blank\">\n\t\t\t\t\t\t<span class=\"elementor-screen-only\">Instagram<\/span>\n\t\t\t\t\t\t<i aria-hidden=\"true\" class=\"fab fa-instagram\"><\/i>\t\t\t\t\t<\/a>\n\t\t\t\t<\/span>\n\t\t\t\t\t\t\t<span class=\"elementor-grid-item\" role=\"listitem\">\n\t\t\t\t\t<a class=\"elementor-icon elementor-social-icon elementor-social-icon-youtube elementor-animation-grow elementor-repeater-item-75dde21\" href=\"https:\/\/www.youtube.com\/watch?v=P9raDgPz29c&#038;t=1s\" target=\"_blank\">\n\t\t\t\t\t\t<span class=\"elementor-screen-only\">Youtube<\/span>\n\t\t\t\t\t\t<i aria-hidden=\"true\" class=\"fab fa-youtube\"><\/i>\t\t\t\t\t<\/a>\n\t\t\t\t<\/span>\n\t\t\t\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<div class=\"elementor-element elementor-element-4f084e5b elementor-widget elementor-widget-text-editor\" data-id=\"4f084e5b\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>Todos os direitos reservados @ Yuri Lima 2025<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>Publications 29. Superdiffusive central limit theorems for geodesic flows on nonpositively curved surfaces With C. Matheus and I. Melbourne. Abstract: We prove a nonstandard central limit theorem and weak invariance principle, with superdiffusive normalisation (tlog t)^{1\/2}, for geodesic flows on a class of nonpositively curved surfaces with flat cylinder. We also prove that correlations decay [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":1263,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"elementor_header_footer","meta":{"om_disable_all_campaigns":false,"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"class_list":["post-1068","page","type-page","status-publish","has-post-thumbnail","hentry"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/yurilima-math.com\/index.php?rest_route=\/wp\/v2\/pages\/1068","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/yurilima-math.com\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/yurilima-math.com\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/yurilima-math.com\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/yurilima-math.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=1068"}],"version-history":[{"count":409,"href":"https:\/\/yurilima-math.com\/index.php?rest_route=\/wp\/v2\/pages\/1068\/revisions"}],"predecessor-version":[{"id":2862,"href":"https:\/\/yurilima-math.com\/index.php?rest_route=\/wp\/v2\/pages\/1068\/revisions\/2862"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/yurilima-math.com\/index.php?rest_route=\/wp\/v2\/media\/1263"}],"wp:attachment":[{"href":"https:\/\/yurilima-math.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=1068"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}