{"id":283,"date":"2024-09-18T18:09:43","date_gmt":"2024-09-18T18:09:43","guid":{"rendered":"http:\/\/localhost:8000\/?page_id=283"},"modified":"2024-09-18T18:10:12","modified_gmt":"2024-09-18T18:10:12","slug":"seminarios-de-probabilidade-2020","status":"publish","type":"page","link":"https:\/\/ppge.im.ufrj.br\/en\/seminarios-de-probabilidade-2020\/","title":{"rendered":"Semin\u00e1rios de probabilidade \u2013 2020"},"content":{"rendered":"<div class=\"fusion-fullwidth fullwidth-box fusion-builder-row-1 fusion-flex-container has-pattern-background has-mask-background nonhundred-percent-fullwidth non-hundred-percent-height-scrolling gradient-container-1\" style=\"--awb-border-radius-top-left:0px;--awb-border-radius-top-right:0px;--awb-border-radius-bottom-right:0px;--awb-border-radius-bottom-left:0px;--awb-flex-wrap:wrap;\" ><div class=\"fusion-builder-row fusion-row fusion-flex-align-items-flex-start fusion-flex-content-wrap\" style=\"max-width:1248px;margin-left: calc(-4% \/ 2 );margin-right: calc(-4% \/ 2 );\"><div class=\"fusion-layout-column fusion_builder_column fusion-builder-column-0 fusion_builder_column_1_1 1_1 fusion-flex-column\" style=\"--awb-bg-size:cover;--awb-width-large:100%;--awb-margin-top-large:0px;--awb-spacing-right-large:1.92%;--awb-margin-bottom-large:20px;--awb-spacing-left-large:1.92%;--awb-width-medium:100%;--awb-order-medium:0;--awb-spacing-right-medium:1.92%;--awb-spacing-left-medium:1.92%;--awb-width-small:100%;--awb-order-small:0;--awb-spacing-right-small:1.92%;--awb-spacing-left-small:1.92%;\"><div class=\"fusion-column-wrapper fusion-column-has-shadow fusion-flex-justify-content-flex-start fusion-content-layout-column\"><div class=\"fusion-title title fusion-title-1 sep-underline sep-solid fusion-title-text fusion-title-size-two\" style=\"--awb-margin-top-small:10px;--awb-margin-right-small:0px;--awb-margin-bottom-small:10px;--awb-margin-left-small:0px;--awb-sep-color:var(--awb-color6);\"><h2 class=\"fusion-title-heading title-heading-left\" style=\"margin:0;text-transform:uppercase;text-shadow:0px #282828;\">Semin\u00e1rios de probabilidade \u2013 2020<\/h2><\/div><div class=\"fusion-separator fusion-full-width-sep\" style=\"align-self: center;margin-left: auto;margin-right: auto;margin-top:20px;margin-bottom:10px;width:100%;\"><\/div><div class=\"fusion-text fusion-text-1\"><div class=\"auto-format ui--animation\">\n<p><strong>Coordena\u00e7\u00e3o:\u00a0<\/strong>Professor\u00a0<a href=\"http:\/\/www.dme.ufrj.br\/?page_id=2698\" target=\"_blank\" rel=\"noopener\">Guilherme Ost<\/a>\u00a0e Professora\u00a0<a href=\"http:\/\/www.dme.ufrj.br\/?page_id=1756\" target=\"_blank\" rel=\"noopener\">Maria Eulalia Vares<\/a><\/p>\n<div class=\"auto-format ui--animation\">\n<p>Devido \u00e0 pandemia de coronav\u00edrus, as palestras ocorrer\u00e3o no ambiente virtual gratuito do Google Meet (<a href=\"https:\/\/meet.google.com\/nxh-optr-wtq\">https:\/\/meet.google.com\/nxh-optr-wtq<\/a>) durante os pr\u00f3ximos meses. As palestras ocorrer\u00e3o\u00a0<b>\u00e0s segundas-feiras \u00e0s 15h<\/b>, a menos de algumas exce\u00e7\u00f5es devidamente indicadas.<\/p>\n<\/div>\n<\/div>\n<\/div><div class=\"fusion-separator fusion-full-width-sep\" style=\"align-self: center;margin-left: auto;margin-right: auto;margin-top:20px;margin-bottom:10px;width:100%;\"><div class=\"fusion-separator-border sep-single sep-solid\" style=\"--awb-height:20px;--awb-amount:20px;--awb-sep-color:var(--awb-color5);border-color:var(--awb-color5);border-top-width:1px;\"><\/div><\/div><\/div><\/div><div class=\"fusion-layout-column fusion_builder_column fusion-builder-column-1 fusion_builder_column_1_1 1_1 fusion-flex-column\" style=\"--awb-bg-size:cover;--awb-width-large:100%;--awb-margin-top-large:0px;--awb-spacing-right-large:1.92%;--awb-margin-bottom-large:20px;--awb-spacing-left-large:1.92%;--awb-width-medium:100%;--awb-order-medium:0;--awb-spacing-right-medium:1.92%;--awb-spacing-left-medium:1.92%;--awb-width-small:100%;--awb-order-small:0;--awb-spacing-right-small:1.92%;--awb-spacing-left-small:1.92%;\"><div class=\"fusion-column-wrapper fusion-column-has-shadow fusion-flex-justify-content-flex-start fusion-content-layout-column\"><div class=\"fusion-text fusion-text-2\"><p><strong>Lista completa<\/strong><\/p>\n<\/div><div class=\"accordian fusion-accordian\" style=\"--awb-border-size:1px;--awb-icon-size:16px;--awb-content-font-size:14px;--awb-icon-alignment:left;--awb-hover-color:var(--awb-color2);--awb-border-color:var(--awb-color3);--awb-background-color:var(--awb-color1);--awb-divider-color:var(--awb-color3);--awb-divider-hover-color:var(--awb-color3);--awb-icon-color:var(--awb-color1);--awb-title-color:var(--awb-color7);--awb-content-color:var(--awb-color8);--awb-icon-box-color:var(--awb-color8);--awb-toggle-hover-accent-color:var(--awb-color5);--awb-title-font-family:var(--awb-typography1-font-family);--awb-title-font-weight:var(--awb-typography1-font-weight);--awb-title-font-style:var(--awb-typography1-font-style);--awb-title-font-size:16px;--awb-content-font-family:var(--awb-typography4-font-family);--awb-content-font-weight:var(--awb-typography4-font-weight);--awb-content-font-style:var(--awb-typography4-font-style);\"><div class=\"panel-group fusion-toggle-icon-boxed\" id=\"accordion-283-1\"><div class=\"fusion-panel panel-default panel-23c52019719b597ba fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_23c52019719b597ba\"><a aria-expanded=\"false\" aria-controls=\"23c52019719b597ba\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#23c52019719b597ba\" href=\"#23c52019719b597ba\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">14\/12<br \/>\n<em>Random walk based algorithms for generating uniform spanning trees<\/em><br \/>\nGiulio Iacobelli (UFRJ)<\/span><\/a><\/h4><\/div><div id=\"23c52019719b597ba\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_23c52019719b597ba\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--title ui--animation ui--title-bordered text-left\">\n<div class=\"ui--title-holder\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\"><a><span class=\"ui--toggle-title-text heading\">The task of efficiently generating uniform spanning trees of a graph has received much attention. A breakthrough came with Aldous-Broder and Wilson\u2019s algorithms, which can efficiently generate spanning trees based on random walks. In this work, we study the transient behavior of both algorithms. We introduce the notion of branches, which are paths generated by the two algorithms on particular stopping times. This interpretation is used to show a transient equivalence between the two algorithms on complete graphs. This equivalence yields a hybrid approach to generate uniform spanning trees of complete graphs faster than either of the two algorithms. We also propose a two-stage framework to explore this hybrid approach beyond complete graphs, showing its feasibility in some examples.<br \/>\n<\/span><\/a><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-3cf3112e424c1df3b fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_3cf3112e424c1df3b\"><a aria-expanded=\"false\" aria-controls=\"3cf3112e424c1df3b\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#3cf3112e424c1df3b\" href=\"#3cf3112e424c1df3b\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">07\/12<em>Percolation on a randomly stretched lattice<\/em><br \/>\nMarcelo Richard Hil\u00e1rio (UFMG)<\/span><\/a><\/h4><\/div><div id=\"3cf3112e424c1df3b\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_3cf3112e424c1df3b\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\"><a><span class=\"ui--toggle-title-text heading\">We consider a stretched version of the square lattice where the distances between neighboring vertical columns are given by interarrival intervals of a renewal process. Hence, horizontal edges that link vertices in the same pair of vertical columns have a common random length while every vertical edge has length one. Conditioned on the realization of the lattice, we define a bond percolation model where edges are open with probabilities that depend on their length. We relate the question of whether the model undergoes a non-trivial phase transition to the moments of interarrival times of the renewal process governing the distance among columns. We will also discuss some other related percolation models defined on media with similar types of columnar disorder. Based on a joint work with Marcos S\u00e1, Augusto Teixeira and Remy Sanchis.<br \/>\n<\/span><\/a><\/div>\n<div class=\"ui--toggle-content\"><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/youtu.be\/NSqJJP9Ef1c\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-4e93dae301bc68b78 fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_4e93dae301bc68b78\"><a aria-expanded=\"false\" aria-controls=\"4e93dae301bc68b78\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#4e93dae301bc68b78\" href=\"#4e93dae301bc68b78\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">30\/11<em>Importance sampling with adaptive winsorization<\/em><br \/>\nPaulo Orenstein (IMPA)<\/span><\/a><\/h4><\/div><div id=\"4e93dae301bc68b78\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_4e93dae301bc68b78\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">Importance sampling is a widely used technique to estimate the properties of a distribution. The resulting estimator is always unbiased, but may sometimes incur huge or infinite variance. This work investigates trading-off some bias for variance by winsorizing the importance sampling estimator using an adaptive thresholding procedure based on the Balancing Principle (also known as Lepskii\u2019s Method). This provides a principled way to perform winsorization, with finite-sample optimality guarantees and good empirical performance.<\/div>\n<div class=\"ui--toggle-content\">\n<p><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/youtu.be\/4YDuXP7Sd9Q\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-2802c209c6256728b fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_2802c209c6256728b\"><a aria-expanded=\"false\" aria-controls=\"2802c209c6256728b\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#2802c209c6256728b\" href=\"#2802c209c6256728b\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">23\/11<br \/>\n<em>Long range percolation models on oriented trees<\/em><br \/>\nAlexsandro Gallo (UFSCar)<\/span><\/a><\/h4><\/div><div id=\"2802c209c6256728b\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_2802c209c6256728b\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">The objective of the talk is to discuss a long range percolation model on oriented trees which contains, as special cases, models such as the frog model with random lifetime and others we may present if time allows. We will be specially interested in localizing, as precisely as possible, the critical parameters.<\/div>\n<div class=\"ui--toggle-content\"><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/youtu.be\/C-OYmybumGw%7C\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-5673b6b01c3d6c52a fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_5673b6b01c3d6c52a\"><a aria-expanded=\"false\" aria-controls=\"5673b6b01c3d6c52a\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#5673b6b01c3d6c52a\" href=\"#5673b6b01c3d6c52a\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">09\/11<br \/>\n<em>Truncation of long-range percolation model with square non-summable interactions<\/em><br \/>\nBernardo N. Borges de Lima (UFMG)<\/span><\/a><\/h4><\/div><div id=\"5673b6b01c3d6c52a\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_5673b6b01c3d6c52a\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">We consider some problems related to the truncation question in long-range percolation. It is given probabilities that certain long-range oriented bonds are open; assuming that these probabilities are not summable, we ask if the probability of percolation is positive when we truncate the graph, disallowing bonds of range above a possibly large but finite threshold. This question is still open if the set of vertices is $Z^2$. We give some conditions in which the answer is affirmative. One of these results generalize the previous result in [Alves, Hil\u00e1rio, de Lima, Valesin, Journ. Stat. Phys. , 972 (2017)]. Joint work with Alberto M. Campos.<\/div>\n<div class=\"ui--toggle-content\"><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/www.youtube.com\/watch?v=ic9W8EK8Lss&feature=youtu.be\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-4a947636d56482187 fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_4a947636d56482187\"><a aria-expanded=\"false\" aria-controls=\"4a947636d56482187\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#4a947636d56482187\" href=\"#4a947636d56482187\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">26\/10<br \/>\n<em>Self-Switching Markov Chains: emerging dominance phenomena<\/em><br \/>\nGuilherme Ost (UFRJ)<\/span><\/a><\/h4><\/div><div id=\"4a947636d56482187\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_4a947636d56482187\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"auto-format ui--animation\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">In many dynamical systems in nature, the law of the dynamics changes along with the temporal evolution of the system. These changes are often associated with the occurrence of certain events. The timing of occurrence of these events depends, in turn, on the trajectory of the dynamical system itself, making the dynamics of the system and the timing of changes in the dynamics strongly coupled. Naturally, trajectories that take longer to satisfy the event will last longer. Therefore, we expect to observe more frequently the dominant dynamics, the ones that take longer to change in the long run. In this talk, we will present a Markov chain model, called Self-Switching Markov Chain (SSMC), in which the emergence of dominant dynamics can be rigorously addressed. We will discuss conditions and scaling in the SSMC under which we observe with probability one only the subset of dominant dynamics. Moreover, we characterize these dominant dynamics. Furthermore, we show that the switching between dynamics exhibits metastability like property. This is a joint work with Daniel Takahashi (UFRN), Giulio Iacobelli (UFRJ) and Sandro Gallo (UFSCar).<\/div>\n<div class=\"ui--toggle-content\"><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/youtu.be\/sIh4-ZVakc0\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/div>\n<\/div>\n<div class=\"ui--toggle-content\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-961d7c3382b42fe26 fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_961d7c3382b42fe26\"><a aria-expanded=\"false\" aria-controls=\"961d7c3382b42fe26\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#961d7c3382b42fe26\" href=\"#961d7c3382b42fe26\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">19\/10<br \/>\n<em>2D anisotropic KPZ at stationarity<\/em><br \/>\nDirk Erhard (UFBA)<\/span><\/a><\/h4><\/div><div id=\"961d7c3382b42fe26\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_961d7c3382b42fe26\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">The KPZ equation is the stochastic partial differential equation in d space dimensions formally given by partial_t h=Delta h +langle h,Q hrangle +xi, where xi is the so called space time white noise, i.e., a gaussian process with short range correlations, and Q is a d dimensional matrix. This equation was introduced in the physics literature in the late eighties to model stochastic growth phenomena, is moreover connected to (d+1) dimensional directed polymers in a random potential and is supposed to arise as a scaling limit of a large class of interacting particle systems.<\/div>\n<div class=\"ui--toggle-content\">\n<div class=\"auto-format ui--animation\">\n<p>In this talk I will try to explain where this equation comes from, why it is interesting, and how its behaviour depends on the spatial dimension. I will mostly focus on the case of dimension 2, and I will comment on a recent result which contradicts a folklore belief from the physics literature.<br \/>\nThis is based on joint works with Giuseppe Cannizzaro, Philipp Sch\u00f6nbauer and Fabio Toninelli.<\/p>\n<\/div>\n<p><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/youtu.be\/950MtqUvcp0\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/p>\n<\/div>\n<\/div>\n<div class=\"ui--toggle-content\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-6ee0c7fe1d5c0b0c7 fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_6ee0c7fe1d5c0b0c7\"><a aria-expanded=\"false\" aria-controls=\"6ee0c7fe1d5c0b0c7\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#6ee0c7fe1d5c0b0c7\" href=\"#6ee0c7fe1d5c0b0c7\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">28\/09<br \/>\n<em>Integration by Parts and the KPZ Two-Point Function<\/em><br \/>\nLeandro Pimentel (UFRJ)<\/span><\/a><\/h4><\/div><div id=\"6ee0c7fe1d5c0b0c7\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_6ee0c7fe1d5c0b0c7\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">All models in the 1+1 Kardar-Parisi-Zhang (KPZ) universality class have fluctuations that converge under KPZ scaling to a universal Markov process, named the KPZ fixed point. In this talk we consider this universal process starting from a two-sided Brownian motion with an arbitrary diffusion coefficient. We apply the integration by parts formula from Malliavin calculus to establish a key relation between the two-point (correlation) function and the location of the maximum of an Airy process plus a Brownian motion with a negative parabolic drift. Integration by parts also allows us to deduce the density of this location in terms of the second derivative of the variance of the KPZ fixed point. We further develop an adaptation of Malliavin-Stein method that implies asymptotic independence with respect to the initial data.<\/div>\n<div class=\"ui--toggle-content\"><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/youtu.be\/uhoXWvAHw78\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/div>\n<\/div>\n<\/div>\n<div class=\"ui--toggle-content\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-c2afabde1152945ce fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_c2afabde1152945ce\"><a aria-expanded=\"false\" aria-controls=\"c2afabde1152945ce\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#c2afabde1152945ce\" href=\"#c2afabde1152945ce\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">14\/09<br \/>\n<em>Non-equilibrium multi-scale analysis and coexistence in competing first-passage percolation<\/em><br \/>\nAlexandre Stauffer (Roma Tre)<\/span><\/a><\/h4><\/div><div id=\"c2afabde1152945ce\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_c2afabde1152945ce\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">We consider a natural random growth process with competition on Z^d called first-passage percolation in a hostile environment, that consists of two first passage percolation processes FPP_1 and FPP_lambda that compete for the occupancy of sites. Initially FPP_1 occupies the origin and spreads through the edges of Z^d at rate 1, while FPP_lambda is initialised at sites called seeds that are distributed according to a product of Bernoulli measures of parameter p. A seed remains dormant until FPP_1 or FPP_lambda attempts to occupy it, after which it spreads through the edges of Z^d at rate lambda. We will discuss the results known for this model and present a recent proof that the two types can coexist (concurrently produce an infinite cluster) on Z^d. We remark that, though counterintuitive, the above model is not monotone in the sense that adding a seed of FPP_lambda could favor FPP_1.<\/div>\n<div class=\"ui--toggle-content\">\n<div class=\"auto-format ui--animation\">\n<p>A central contribution of our work is the development of a novel multi-scale analysis to analyze this model, which we call a multi-scale analysis with non-equilibrium feedback and which we believe could help analyze other models with non-equilibrium dynamics and lack of monotonicity. A crucial step in our analysis is the addition of some non-local events to the multi-scale framework, and interplaying the non-local events with a by now \u201cstandard\u201d multi-scale renormalization.<\/p>\n<p>Based on a joint work with Tom Finn (Univ. of Bath).<\/p>\n<\/div>\n<p><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/youtu.be\/2JkGDl2f5Ak\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/p>\n<\/div>\n<\/div>\n<div class=\"ui--toggle-content\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-57e2aff9ea338b68a fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_57e2aff9ea338b68a\"><a aria-expanded=\"false\" aria-controls=\"57e2aff9ea338b68a\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#57e2aff9ea338b68a\" href=\"#57e2aff9ea338b68a\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">24\/08<br \/>\n<em>Mixing rates for processes with long-memory<\/em><br \/>\nDaniel Takahashi (UFRN)<\/span><\/a><\/h4><\/div><div id=\"57e2aff9ea338b68a\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_57e2aff9ea338b68a\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\"><a><span class=\"ui--toggle-title-text heading\">Daniel Takahashi (UFRN)<\/span><\/a><\/div>\n<div class=\"ui--toggle-content\">\n<div class=\"auto-format ui--animation\">\n<p>Non-Markovian processes are ubiquitous, but they are much less understood compared to Markov processes. We model non-Markovianity using probability kernels that can depend on its entire history. The continuity rate characterizes how the dependence of kernel on the past decays. One key question is to understand how the mixing rates and decay of correlation are related to the continuity rate. Pollicot (2000) and Bressaud, Fernandez, Galves (1999) showed that if the continuity rate decays as O(1\/n^c), for c &gt; 1, then the correlation also decays as O(1\/n^c). Johansson, Oberg, Pollicott (2007) proved the uniqueness of the stationary measure compatible with kernels with the continuity rate in O(1\/n^c), for c &gt; 1\/2. Moreover, Berger, Hoffman, Sidoravicius (2018) established that there are kennels with multiple compatible measures whenever c &lt; 1\/2. Therefore, the natural question is to understand the mixing rates and correlation decays when c is in [1\/2,1]. In this talk, I will exhibit upper bounds for the mixing rates and correlation decays when the continuity rate decays as O(1\/n^c), for c in (1\/2,1]. If time allows, I will show how to apply the result to prove a new weak invariance principle. This talk is based on joint work with Christophe Gallesco.<\/p>\n<\/div>\n<p><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/www.youtube.com\/watch?v=8Q7KUkuGYp4&amp;t=765s&amp;ab_channel=probabilidadeIm\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/p>\n<\/div>\n<\/div>\n<div class=\"ui--toggle-content\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-8f3005512e7ab1564 fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_8f3005512e7ab1564\"><a aria-expanded=\"false\" aria-controls=\"8f3005512e7ab1564\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#8f3005512e7ab1564\" href=\"#8f3005512e7ab1564\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">10\/08<br \/>\n<em>Spatial Gibbs Random Graphs<\/em><br \/>\nAndressa Cerqueira (UFSCar)<\/span><\/a><\/h4><\/div><div id=\"8f3005512e7ab1564\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_8f3005512e7ab1564\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">In this talk, I will present a Spatial Gibbs Random Graph Model on Z^2 that incorporates the interplay between the statistics of the graph and the underlying space where the vertices are located. For this model, we prove the existence and uniqueness of a measure defined on graphs with vertices in Z^2 as the limit along the measures over graphs with finite vertex set. I will explain how the results are obtained based on a graphical construction of the model as the invariant measure of a birth and death process. This is a joint work with Nancy Garcia.<\/div>\n<div class=\"ui--toggle-content\"><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/www.youtube.com\/watch?v=H53cXpL0TQg&amp;ab_channel=probabilidadeIm\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/div>\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-content\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-89351fa368ea95fda fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_89351fa368ea95fda\"><a aria-expanded=\"false\" aria-controls=\"89351fa368ea95fda\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#89351fa368ea95fda\" href=\"#89351fa368ea95fda\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">27\/07<br \/>\n<em>On the threshold of spread-out contact process percolation<\/em><br \/>\nDaniel Valesin (University of Groningen)<\/span><\/a><\/h4><\/div><div id=\"89351fa368ea95fda\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_89351fa368ea95fda\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">We study the stationary distribution of the (spread-out) d-dimensional contact process from the point of view of site percolation. In this process, vertices of Z^d can be healthy (state 0) or infected (state 1). With rate one infected individuals recover, and with rate lambda they transmit the infection to some other vertex chosen uniformly within a ball of radius R. The classical phase transition result for this process states that there is a critical value lambda_c(R) such that the process has a non-trivial stationary distribution if and only if lambda &gt; lambda_c(R). In configurations sampled from this stationary distribution, we study nearest neighbor site percolation of the set of infected sites; the associated percolation threshold is denoted lambda_p(R). We prove that lambda_p(R) converges to 1\/(1 p_c) as R tends to infinity, where p_c is the threshold for Bernoulli site percolation on Z^d. As a consequence, we prove that lambda_p(R) &gt; lambda_c(R) for large enough R, answering an open question of [Liggett, Steif, AIHP, 2006] in the spread-out case. Joint work with Bal\u00e1zs R\u00e1th.<\/div>\n<div class=\"ui--toggle-content\"><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/www.youtube.com\/watch?v=QEZ4vVn_mSU&amp;ab_channel=probabilidadeIm\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/div>\n<\/div>\n<div class=\"ui--toggle-content\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-813063b4533317dd4 fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_813063b4533317dd4\"><a aria-expanded=\"false\" aria-controls=\"813063b4533317dd4\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#813063b4533317dd4\" href=\"#813063b4533317dd4\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">13\/07<br \/>\n<em>Quantification under prior probability shift: the ratio estimator and its extensions<\/em><br \/>\nRafael Izbicki (UFSCar)<\/span><\/a><\/h4><\/div><div id=\"813063b4533317dd4\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_813063b4533317dd4\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">The quantification problem consists of determining the prevalence of a given label in a target population using labels from a sample from the training population. A common assumption in this situation is that of prior probability shift, that is, once the labels are known, the distribution of the features is the same in the training and target populations. In this paper, we derive a new lower bound for the risk of the quantification problem under the prior shift assumption. Complementing this lower bound, we present a new approximately minimax class of estimators, ratio estimators, which generalize several previous proposals in the literature. Using a weaker version of the prior shift assumption, which can be tested, we show that ratio estimators can be used to build confidence intervals for the quantification problem. We also extend the ratio estimator so that it can:(i) incorporate labels from the target population, when they are available and (ii) estimate how the prevalence of positive labels varies according to a function of certain covariates.<\/div>\n<div class=\"ui--toggle-content\"><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/youtu.be\/w8Ic29bzXyE\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/div>\n<\/div>\n<div class=\"ui--toggle-content\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-1e1d6d7e7e6403676 fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_1e1d6d7e7e6403676\"><a aria-expanded=\"false\" aria-controls=\"1e1d6d7e7e6403676\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#1e1d6d7e7e6403676\" href=\"#1e1d6d7e7e6403676\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">29\/06<br \/>\n<em>Brownian motion in inverse-square Poisson potential<\/em><br \/>\nRenato Soares dos Santos (UFMG)<\/span><\/a><\/h4><\/div><div id=\"1e1d6d7e7e6403676\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_1e1d6d7e7e6403676\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">We consider the parabolic Anderson model in d-dimensional space, i.e., the stochastic heat equation with multiplicative potential, with a random attractive potential having inverse-square singularities on the points of a standard Poisson point process. We study existence and large-time asymptotics of positive solutions via Feynman-Kac representation.<\/div>\n<div class=\"ui--toggle-content\"><a class=\"btn btn-normal btn-icon-left btn-primary ui--animation\" href=\"https:\/\/youtu.be\/FlDk8mu3Hrk\" target=\"_blank\" rel=\"noopener\">Assista \u00e0 palestra no Youtube<\/a><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-92323a289fd77e906 fusion-toggle-has-divider\" style=\"--awb-title-color:var(--awb-color8);--awb-content-color:var(--awb-color8);\"><div class=\"panel-heading\"><h4 class=\"panel-title toggle\" id=\"toggle_92323a289fd77e906\"><a aria-expanded=\"false\" aria-controls=\"92323a289fd77e906\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-283-1\" data-target=\"#92323a289fd77e906\" href=\"#92323a289fd77e906\"><span class=\"fusion-toggle-icon-wrapper\" aria-hidden=\"true\"><i class=\"fa-fusion-box active-icon awb-icon-minus\" aria-hidden=\"true\"><\/i><i class=\"fa-fusion-box inactive-icon awb-icon-plus\" aria-hidden=\"true\"><\/i><\/span><span class=\"fusion-toggle-heading\">09\/03<br \/>\n<em>Probabilistic model for integer partitions<\/em><br \/>\nStella Brassesco (Instituto Venezolano de Investigaciones Cient\u00edficas)<\/span><\/a><\/h4><\/div><div id=\"92323a289fd77e906\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_92323a289fd77e906\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle ui--animation clearfix ui--toggle-state-opened\">\n<div class=\"ui--toggle-content\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">A family of independent random variables can be associated to the sequence p(n), which counts the number of partitions of a natural number n. The sum of those variables, suitably normalized, can be seen to converge to a Gaussian random variable, which suggests a method to obtain detailed asymptotics for p(n) an n goes to infinity. Moreover, the representation is useful to deduce asymptotic properties when the uniform distribution is considered on the set of partitions of n. The problem is related with questions arising in several contexts.<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"open","template":"100-width.php","meta":{"footnotes":""},"class_list":["post-283","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/pages\/283","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/comments?post=283"}],"version-history":[{"count":3,"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/pages\/283\/revisions"}],"predecessor-version":[{"id":287,"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/pages\/283\/revisions\/287"}],"wp:attachment":[{"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/media?parent=283"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}