{"id":289,"date":"2024-09-18T18:26:12","date_gmt":"2024-09-18T18:26:12","guid":{"rendered":"http:\/\/localhost:8000\/?page_id=289"},"modified":"2024-09-18T18:28:17","modified_gmt":"2024-09-18T18:28:17","slug":"seminarios-de-probabilidade-2019","status":"publish","type":"page","link":"https:\/\/ppge.im.ufrj.br\/en\/seminarios-de-probabilidade-2019\/","title":{"rendered":"Semin\u00e1rios de probabilidade \u2013 2019"},"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 2019<\/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>Professora Maria Eulalia Vares<\/p>\n<p>As palestras ocorrerem na sala B106-b nas segundas-feiras \u00e0s 15h30, a menos de algumas exce\u00e7\u00f5es devidamente indicadas.<\/p>\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-289-1\"><div class=\"fusion-panel panel-default panel-609c6e8f44a593b67 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_609c6e8f44a593b67\"><a aria-expanded=\"false\" aria-controls=\"609c6e8f44a593b67\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#609c6e8f44a593b67\" href=\"#609c6e8f44a593b67\"><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\">25\/11<br \/>\n<em>Dependent Mixtures: Modelling cell lineages<\/em><br \/>\nCarlos Tadeu Pagani Zanini (IM-UFRJ)<\/span><\/a><\/h4><\/div><div id=\"609c6e8f44a593b67\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_609c6e8f44a593b67\"><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\">\n<div class=\"ui--toggle-title\">Cell lineage data comes from single-cell transcriptomics and it is used to recover the evolutionary path of cells in a given environment. The different evolutionary stages of the cells can be probabilistically described by distinct components in a mixture model. This work proposes a Bayesian dependent mixture model where the dependence on the components of the mixture explicitly incorporates the biological structure that characterizes cell lineage applications. We use a random tree structure (Minimum Spanning Tree) not only to explain the snapshot in the latent space of the continuous development of cells from its initial stage into mature differentiated cells, but also to model the dependence structure between the clusters of cells. Regularization is incorporated in the form of a prior penalization on trees with too many nodes or with redundant edges. Consequently, the model assumes the partition of cells to depend on the lineage structure, which is more biologically reasonable then the usual multistep approach in which partitions are estimated disregarding the underlying tree structure that characterizes cell lineage data. We are able to provide full inference (with uncertainty captured by the posterior samples obtained through MCMC) on the clusters of cells (including number of clusters), on the underlying tree structure and also on pseudotimes.<\/div>\n<div class=\"ui--toggle-content\">\n<div class=\"auto-format ui--animation\">\n<p>Authors: Zanini, C. T. P, Paulon, G., Mueller, P.<\/p>\n<\/div>\n<\/div>\n<p><a><span class=\"ui--toggle-title-text heading\">\u00a0<\/span><\/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-685ad897c76e24086 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_685ad897c76e24086\"><a aria-expanded=\"false\" aria-controls=\"685ad897c76e24086\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#685ad897c76e24086\" href=\"#685ad897c76e24086\"><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\">11\/11<br \/>\n<em>Percolation on a randomly stretched lattice<\/em><br \/>\nDaniel Ungaretti Borges (Unicamp)<\/span><\/a><\/h4><\/div><div id=\"685ad897c76e24086\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_685ad897c76e24086\"><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\">We will discuss the two-dimensional simple random walk conditioned on never hitting the origin, which is, formally speaking, the Doob\u2019s h-transform of the simple random walk with respect to the potential kernel. This random walk is the main building-block of the construction of random interlacements on the plane introduced by Comets, Popov and Vachkovskaia. However, this walk has become an interesting object on its own. To justify this claim we present a few of its properties, citing some of the current literature and presenting the results of a recent joint work with Serguei Popov (UNICAMP) and Leonardo Rolla (UBA\/NYU Shanghai).<\/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-07d5b2d88d1266ca5 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_07d5b2d88d1266ca5\"><a aria-expanded=\"false\" aria-controls=\"07d5b2d88d1266ca5\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#07d5b2d88d1266ca5\" href=\"#07d5b2d88d1266ca5\"><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\/10<br \/>\n<em>The Luce model with replicas<em><br \/>\nJos\u00e9 Heleno Faro (Insper)<\/span><\/a><\/h4><\/div><div id=\"07d5b2d88d1266ca5\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_07d5b2d88d1266ca5\"><div class=\"panel-body toggle-content fusion-clearfix\"><\/em><\/em><\/p>\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\"><a><span class=\"ui--toggle-title-text heading\">Jos\u00e9 Heleno Faro (Insper)<\/span><\/a><\/div>\n<div class=\"ui--toggle-content\">\n<div class=\"auto-format ui--animation\">\n<p>We propose the notion of replicas in the context of discrete choices and introduce axioms that support which we call the Luce model with replicas. Unlike other relations proposed in the literature that can deal with the duplicates problem, ours entails replicas as a combination of duplicates and stochastically perfect substitutes, which induces a partition of the entire set of alternatives into endogeneous nests of replicas. Our model is less restrictive than Luce.s model and more parsimonious than the available models that may deal with the violation of the constant-ratio rule anticipated by Debreu (1960).<\/p>\n<\/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><\/div><\/div><div class=\"fusion-panel panel-default panel-5bdb3321bebfa17d7 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_5bdb3321bebfa17d7\"><a aria-expanded=\"false\" aria-controls=\"5bdb3321bebfa17d7\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#5bdb3321bebfa17d7\" href=\"#5bdb3321bebfa17d7\"><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\/09<br \/>\n<em>Functional It\u00f4 Calculus and Applications to Stochastic Control<\/em><br \/>\nYuri Saporito (EMAp-FGV)<\/span><\/a><\/h4><\/div><div id=\"5bdb3321bebfa17d7\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_5bdb3321bebfa17d7\"><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\">In this talk we will review the recent developments on Functional It\u00f4 calculus, FITO in short. Created (or discovered) by Bruno Dupire and published in a seminal paper in 2009, this calculus is a generalization of It\u00f4\u2019s classical theory and allows us to examine models where the history of certain factors plays an important role. We will present the general theory and survey the theoretical unfolding of FITO. As an application, we will show how this theory allows us to consider stochastic control problems with path-dependence influence of the control in the dynamics of the state process.<\/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-22e86cdc10a529f0f 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_22e86cdc10a529f0f\"><a aria-expanded=\"false\" aria-controls=\"22e86cdc10a529f0f\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#22e86cdc10a529f0f\" href=\"#22e86cdc10a529f0f\"><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\">16\/09<br \/>\n<em>A non-local and non-linear SPDE<\/em><br \/>\nLeandro Chiarini Medeiros (IMPA)<\/span><\/a><\/h4><\/div><div id=\"22e86cdc10a529f0f\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_22e86cdc10a529f0f\"><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\">\n<div class=\"ui--toggle-title\">In this presentation, we will discuss the existence of a local solution to the equation<\/div>\n<div class=\"ui--toggle-content\">\n<div class=\"auto-format ui--animation\">\n<p>$$<br \/>\n\\partial X = -(-\\Delta)^ X \u2013\u00a0\\sinh(\\gamma X) +\u00a0\\xi,<br \/>\n$$<br \/>\nwhere $(-\\Delta)^$ is the half-laplacian, and $\\xi$ is the space-time white noise. As the solution is not point-wise welldefined function, we will have to define the meaning of $\\sinh(\\gamma X)$. We will also discuss the basic ideas between da Pratto Debusche approach to non-linear SPDE's and more modern techniques, such as regularity structures.<\/p>\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-23c50082426657a1f 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_23c50082426657a1f\"><a aria-expanded=\"false\" aria-controls=\"23c50082426657a1f\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#23c50082426657a1f\" href=\"#23c50082426657a1f\"><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\/09<br \/>\n<em>Converg\u00eancia em um Modelo de Filas com Servi\u00e7os Brownianos<\/em><br \/>\nLeandro P. R. Pimentel (IM-UFRJ)<\/span><\/a><\/h4><\/div><div id=\"23c50082426657a1f\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_23c50082426657a1f\"><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\">\n<div class=\"ui--toggle-title\">A teoria de filas \u00e9 um ramo da probabilidade que estuda sistemas de atendimento onde temos um processo estoc\u00e1stico que descreve a chegada de clientes de forma ordenada a uma unidade de atendimento, formando-se filas de espera, e um outro que descreve o tempo atribu\u00eddo a cada servi\u00e7o. Nessa apresenta\u00e7\u00e3o iremos estudar propriedades assimpt\u00f3ticas de um sistema onde clientes passam por uma s\u00e9rie de filas em ordem, e os tempos de atendimento s\u00e3o dados por movimentos Brownianos.<\/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-fa523bf232e4067fb 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_fa523bf232e4067fb\"><a aria-expanded=\"false\" aria-controls=\"fa523bf232e4067fb\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#fa523bf232e4067fb\" href=\"#fa523bf232e4067fb\"><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\/08<br \/>\n<em>Assinaturas de Revistas e Desconto Intertemporal: Evid\u00eancias do Mercado Brasileiro<\/em><br \/>\nEduardo Ferioli Gomes (IME-UFF)<\/span><\/a><\/h4><\/div><div id=\"fa523bf232e4067fb\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_fa523bf232e4067fb\"><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\">O presente trabalho apresenta uma abordagem integrada para o processo de discrimina\u00e7\u00e3o de pre\u00e7os para assinaturas de revistas que contempla tamb\u00e9m a renda das editoras provenientes da venda de publicidade. Segundo Scott-Morton (2005) o n\u00edvel de benef\u00edcio de longo prazo que cada publica\u00e7\u00e3o oferece seria inversamente proporcional ao desconto oferecido pela editora na assinatura. Entretanto, n\u00e3o foram encontradas evid\u00eancias emp\u00edricas deste comportamento ao serem consideradas outras caracter\u00edsticas das publica\u00e7\u00f5es na an\u00e1lise econom\u00e9trica em um mercado no qual os pontos de venda s\u00e3o muito mais disseminados. Em particular, o horizonte de assinatura n\u00e3o apresentou um papel relevante no grau de desconto da assinatura com rela\u00e7\u00e3o ao pre\u00e7o de face. Ao contr\u00e1rio, uma an\u00e1lise explorat\u00f3ria feita por componentes principais, posteriormente confirmadas pelo modelo de regress\u00e3o, sugere a exist\u00eancia de um processo multidimensional de discrimina\u00e7\u00e3o de pre\u00e7os que envolve o desconto nas assinaturas e no pre\u00e7o de publicidade. Este \u00e9 um trabalho em conjunto com Marcelo Resende (IE \u2013 UFRJ) e publicado na 38\u00aa edi\u00e7\u00e3o do Economics Bulletin.<\/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-b3748b0446ab800af 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_b3748b0446ab800af\"><a aria-expanded=\"false\" aria-controls=\"b3748b0446ab800af\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#b3748b0446ab800af\" href=\"#b3748b0446ab800af\"><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\">12\/08<br \/>\n<em>Disordered Bose-Einstein condensate in hard walls trap<\/em><br \/>\nNami Fux Svaiter (CBPF)<\/span><\/a><\/h4><\/div><div id=\"b3748b0446ab800af\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_b3748b0446ab800af\"><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 discuss the effects of quenched disorder in a dilute Bose-Einstein condensate confined in a hard walls trap. Starting from the disordered Gross-Pitaevskii functional, we obtain a representation for the quenched free energy as a series of integer moments of the partition function. Positive and negative disorder-dependent effective coupling constants appear in the integer moments. Going beyond the mean-field approximation, we compute the static two-point correlation functions at first-order in the positive effective coupling constants. We obtain the combined contributions of effects due to boundary conditions and disorder in this weakly disordered condensate. The ground state renormalized density profile of the condensate is presented. We also discuss the appearance of metastable and true ground states for strong disorder, when the effective coupling constants become negative.<\/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-05199ff10e2976874 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_05199ff10e2976874\"><a aria-expanded=\"false\" aria-controls=\"05199ff10e2976874\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#05199ff10e2976874\" href=\"#05199ff10e2976874\"><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\">01\/07<br \/>\n<em>Recorr\u00eancia, transi\u00eancia e balisticidade de passeios aleat\u00f3rios geradores de \u00e1rvores<\/em><br \/>\nGlauco Valle (IM-UFRJ)<\/span><\/a><\/h4><\/div><div id=\"05199ff10e2976874\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_05199ff10e2976874\"><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\">O comportamento assint\u00f3tico de classes de Passeios aleat\u00f3rios n\u00e3o markovianos ou em ambiente aleat\u00f3rios \u00e9 um tema central em teoria das probabilidades e aplica\u00e7\u00f5es. Os passeios que iremos considerar neste semin\u00e1rio s\u00e3o tanto n\u00e3o markovianos quanto sua evolu\u00e7\u00e3o pode ser descrita em fun\u00e7\u00e3o de um ambiente aleat\u00f3rio. Esses passeios s\u00e3o chamados de passeios aleat\u00f3rios geradores de \u00e1rvores e podem ser descritos da seguinte forma: (1) Consideramos um passeio aleat\u00f3rio em um grafo G com escolhas uniformes entre vizinhos pr\u00f3ximos a cada transi\u00e7\u00e3o; (2) ap\u00f3s um certo n\u00famero L (fixo) de passos um n\u00famero de aleat\u00f3rio de v\u00e9rtices s\u00e3o criados e anexados \u00e0 posi\u00e7\u00e3o atual do passeio; (1) e (2) se repetem recursivamente. Estudaremos o comportamento assint\u00f3tico desses passeios em fun\u00e7\u00e3o do valor de L, estabelecendo propriedades como recorr\u00eancia, transi\u00eancia e balisticidade.<\/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-745d34c923dd4d7ec 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_745d34c923dd4d7ec\"><a aria-expanded=\"false\" aria-controls=\"745d34c923dd4d7ec\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#745d34c923dd4d7ec\" href=\"#745d34c923dd4d7ec\"><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\/06<br \/>\n<em>A zero range process with rapidly growing rates<\/em><br \/>\nEnrique D. Andjel (Aix Marseille \/ IMPA)<\/span><\/a><\/h4><\/div><div id=\"745d34c923dd4d7ec\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_745d34c923dd4d7ec\"><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\">Most constructions of the zero range process assume that the rate at which a particle leaves a site grows at most linearly with the number of particles present at that site. We provide a method to construct a zero range processes with super-linear rates on $mathbb^d $ when either the initial distribution is translation invariant or d=1 and only nearest neighbor jumps are allowed.<\/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-ed243a4379ace6d80 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_ed243a4379ace6d80\"><a aria-expanded=\"false\" aria-controls=\"ed243a4379ace6d80\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#ed243a4379ace6d80\" href=\"#ed243a4379ace6d80\"><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\">03\/06<br \/>\n<em>Sparse space-time models: Concentration inequalities and Lasso<\/em><br \/>\nGuilherme Ost (IM-UFRJ)<\/span><\/a><\/h4><\/div><div id=\"ed243a4379ace6d80\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_ed243a4379ace6d80\"><div class=\"panel-body toggle-content fusion-clearfix\">\n<div class=\"ui--toggle-title\">\n<div class=\"ui--toggle-title\">Inspired by Kalikow-type decompositions, we introduce a new stochastic model describing a network of interacting neurons. For such class we establish oracle inequalities for Lasso methods and restricted eigenvalue properties for the associated Gram matrix with high probability. These results hold even if the network is only partially observed. The main argument rely on the fact that concentration inequalities can easily be derived whenever the transition probabilities of the underlying process admit a sparse space-time representation.<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-d53bc8f235a9be0a5 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_d53bc8f235a9be0a5\"><a aria-expanded=\"false\" aria-controls=\"d53bc8f235a9be0a5\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#d53bc8f235a9be0a5\" href=\"#d53bc8f235a9be0a5\"><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\/05<br \/>\n<em>Critical scaling for an anisotropic percolation model on Z^2<\/em><br \/>\nMaria Eulalia Vares (IM-UFRJ)<\/span><\/a><\/h4><\/div><div id=\"d53bc8f235a9be0a5\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_d53bc8f235a9be0a5\"><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\">\n<div class=\"ui--toggle-title\">We consider an anisotropic finite-range bond percolation model on $mathbb^2$. On each horizontal layer $H_i={(x,i)colon x in mathbb}$ we have edges $langle (x,i),(y,i)rangle$ for $1 le |x-y|le N$. There are also vertical edges connecting two nearest neighbor vertices on distinct lines $langle (x,i),(x,i+1)rangle$ for $x,i in mathbb$. On this graph we consider the following anisotropic independent percolation model: horizontal edges are open with probability $1\/(2N)$, while vertical edges are open with probability $epsilon$ to be suitably tuned as $N$ grows to infinity. The main result tells that if $epsilon = kappa N^$, then we see a phase transition in $kappa$: there exist positive and finite constants $C_1, C_2$ so that there is no percolation if $kappa <c_1$ while=\"\" percolation=\"\" occurs=\"\" for=\"\" $kappa=\"\">C_2$.<\/c_1$><\/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>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-475b3082001c75a4d 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_475b3082001c75a4d\"><a aria-expanded=\"false\" aria-controls=\"475b3082001c75a4d\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#475b3082001c75a4d\" href=\"#475b3082001c75a4d\"><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\/05<br \/>\n<em>On the singularity of random symmetric matrices<\/em><br \/>\nLet\u00edcia Mattos (IMPA)<\/span><\/a><\/h4><\/div><div id=\"475b3082001c75a4d\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_475b3082001c75a4d\"><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\">\n<div class=\"ui--toggle-title\">A well-known conjecture states that a random symmetric n-by-n matrix with entries in  is singular with probability 2^. In this talk we will show that the probability of this event is at most 2^, improving the best known bound 2^, which was obtained recently by Ferber and Jain. The main new ingredient is an inverse Littlewood\u2013Offord theorem in Z_p^n that applies under very mild conditions, whose statement is inspired by the method of hypergraph containers. This is a joint work with Marcelo Campos, Robert Morris and Natasha Morrison.<\/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>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-042d84babbfc2f1e5 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_042d84babbfc2f1e5\"><a aria-expanded=\"false\" aria-controls=\"042d84babbfc2f1e5\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#042d84babbfc2f1e5\" href=\"#042d84babbfc2f1e5\"><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\">01\/04<br \/>\n<em>Anisotropic bootstrap percolation<\/em><br \/>\nDaniel Ricardo B. Tordecilla (IMPA)<\/span><\/a><\/h4><\/div><div id=\"042d84babbfc2f1e5\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_042d84babbfc2f1e5\"><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\">\n<div class=\"ui--toggle-title\">Bootstrap percolation is a monotone version of the Glauber dynamics of the Ising model of ferromagnetism. In this talk we will consider anisotropic bootstrap models, which are three-dimensional analogues of a family of (two-dimensional) processes studied by Duminil-Copin, van Enter and Hulshof. In these models the underlying graph $G$ has vertex set $[L]^3$, and the neighbourhood of each vertex consists of the $a_i$ nearest neighbours in the $e_i$-direction for each $i in $, where $a_1le a_2le a_3$. Given an initial configuration in $^$, the system evolves in discrete time in the following way: the state of a vertex $v$ changes from $0$ to $1$ when it has at least $r$ neighbours in state $1$. The initial state is usually chosen to be the product of Bernoulli measures with density $p$, and the main question is to determine the so-called  $L_c(p)$, for small values of $p$.<\/div>\n<div class=\"ui--toggle-content\">\n<div class=\"auto-format ui--animation\">\n<p>It turns out that $L_c(p)$ is polynomial if $r le a_3$, exponential if $a_3 < r le a_2 + a_3$, doubly exponential if $a_2 + a_3 < r le a_1 + a_2 + a_3$, and infinite if $r > a_1 + a_2 + a_3$. In this talk we will focus on the case $r = a_3 + 1$, and show how to determine $log L_c(p)$ up to a constant factor. The main new tool, which we call the , allows one to reduce the problem to proving an exponential decay property for a certain two-dimensional model whose behaviour resembles site percolation.<\/p>\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>\n<\/div>\n<\/div>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-082a3f17b97479c65 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_082a3f17b97479c65\"><a aria-expanded=\"false\" aria-controls=\"082a3f17b97479c65\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#082a3f17b97479c65\" href=\"#082a3f17b97479c65\"><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\">18\/03<br \/>\n<em>A martingale approach to convergence to the Kingman's coalescents<\/em><br \/>\nEnrique Chavez Sarmiento (IMPA)<\/span><\/a><\/h4><\/div><div id=\"082a3f17b97479c65\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_082a3f17b97479c65\"><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\">\n<div class=\"ui--toggle-title\">We consider the following dynamic. We start with a fix number of la-beled, i.i.d. Markov chains over a finite state space, let the time pass, and when two chains meet, they behave as one chain. This dynamic induces a process in the set of partitions of the first natural numbers. We are interested in the asymptotic behavior of this process. On the late eighties J. T. Cox obtained some limit theo rems for coalescing random walks on the discrete torus, when the Markov chains we considered before are simple random walks and we start with one random walk in each vertex of the torus. Since then the asymptotic behavior of the coa-lescence time, the first time all the chains meet, has been the subject of several papers. And the result of Cox has being extended in different ways. In this talk we describe some of these extensions, and use a martingale approach to prove, under certain conditions, the convergence of the process in the set of partitions of the first natural numbers, we described before, to the Kingman\u2019s coalescent start-ing from a finite number of partitions.<\/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>\n<\/div><\/div><\/div><div class=\"fusion-panel panel-default panel-5e4ee992a60da3e85 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_5e4ee992a60da3e85\"><a aria-expanded=\"false\" aria-controls=\"5e4ee992a60da3e85\" role=\"button\" data-toggle=\"collapse\" data-parent=\"#accordion-289-1\" data-target=\"#5e4ee992a60da3e85\" href=\"#5e4ee992a60da3e85\"><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\">11\/03<br \/>\n<em>Metastability for the one-dimensional contact process with two types of particles and priorities<\/em><br \/>\nMariela Pent\u00f3n Machado (UFRJ)<\/span><\/a><\/h4><\/div><div id=\"5e4ee992a60da3e85\" class=\"panel-collapse collapse \" aria-labelledby=\"toggle_5e4ee992a60da3e85\"><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\">\n<div class=\"ui--toggle-title\">We consider a symmetric finite-range contact process on Z with two types of particles (or infections), which propagate according to the same supercritical rate and die (or heal) at rate 1. Particles of type 1 can occupy any site in (-infty,0]that is empty or occupied by a particle of type 2 and, analogously, particles of type 2 can occupy any site in [1,+infty) that is empty or occupied by a particle of type 1. We consider the model restricted to a finite interval [-N+1,N] (on the integers). If the initial configuration is (-N,0] fully occupied by type 1 particles and [1,N) fully occupied by type 2 particles, we prove that this dynamic presents two metastable states: one with the two species and the other one with the family that survives the competition.<\/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>\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-289","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/pages\/289","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=289"}],"version-history":[{"count":3,"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/pages\/289\/revisions"}],"predecessor-version":[{"id":292,"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/pages\/289\/revisions\/292"}],"wp:attachment":[{"href":"https:\/\/ppge.im.ufrj.br\/en\/wp-json\/wp\/v2\/media?parent=289"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}