{"id":2,"date":"2019-03-13T10:09:53","date_gmt":"2019-03-13T09:09:53","guid":{"rendered":"http:\/\/web.infn.it\/FRGIM\/?page_id=2"},"modified":"2019-04-24T14:53:09","modified_gmt":"2019-04-24T12:53:09","slug":"scientific-project","status":"publish","type":"page","link":"https:\/\/web.infn.it\/FRGIM\/scientific-project\/","title":{"rendered":"Scientific Project"},"content":{"rendered":"\n<div class=\"alignwide\"><div id=\"metaslider-id-342\" style=\"width: 100%;\" class=\"ml-slider-3-108-0 metaslider metaslider-flex metaslider-342 ml-slider has-dots-nav ms-theme-default\" role=\"region\" aria-label=\"New Slideshow\" data-height=\"400\" data-width=\"700\">\n    <div id=\"metaslider_container_342\">\n        <div id=\"metaslider_342\">\n            <ul class='slides'>\n                <li style=\"display: block; width: 100%;\" class=\"slide-344 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:25:38\" data-filename=\"Black_hole_NASA-700x400.jpg\" data-slide-type=\"image\"><a href=\"https:\/\/commons.wikimedia.org\/w\/index.php?curid=41498\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/Black_hole_NASA-700x400.jpg\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-344 msDefaultImage\" title=\"Black_hole_NASA\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">An artist's impression of a supermassive black hole devouring matter from an accretion disc.<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-346 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:31:10\" data-filename=\"bubble-chamber-bebc-600x342.jpg\" data-slide-type=\"image\"><a href=\"https:\/\/home.cern\/news\/news\/experiments\/seeing-invisible-event-displays-particle-physics\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/bubble-chamber-bebc-600x342.jpg\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-346 msDefaultImage\" title=\"bubble-chamber-bebc\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">Charged particles moving in the hydrogen-neon liquid  of the Big European Bubble Chamber.<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-348 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:33:06\" data-filename=\"Ilc_9yr_moll4096-700x400.png\" data-slide-type=\"image\"><a href=\"http:\/\/map.gsfc.nasa.gov\/media\/121238\/index.html\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/Ilc_9yr_moll4096-700x400.png\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-348 msDefaultImage\" title=\"Ilc_9yr_moll4096\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">The detailed, all-sky picture of the infant universe created from nine years of WMAP data.\n<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-350 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:36:03\" data-filename=\"Structure_of_the_Universe-700x400.jpg\" data-slide-type=\"image\"><a href=\"http:\/\/www.nasa.gov\/mission_pages\/hubble\/science\/hst_img_20080520.html\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/Structure_of_the_Universe-700x400.jpg\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-350 msDefaultImage\" title=\"Structure_of_the_Universe\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">Matter (primarily dark matter) distribution in a cubic section of the universe.<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-352 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:38:32\" data-filename=\"Interplay-of-active-processes-modulates-tension-and-drives-phase-transition-in-self-renewing-motor-ncomms10323-s2_ogv-700x400.jpg\" data-slide-type=\"image\"><a href=\"https:\/\/commons.wikimedia.org\/wiki\/File:Interplay-of-active-processes-modulates-tension-and-drives-phase-transition-in-self-renewing-motor-ncomms10323-s2.ogv\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/Interplay-of-active-processes-modulates-tension-and-drives-phase-transition-in-self-renewing-motor-ncomms10323-s2_ogv-700x400.jpg\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-352 msDefaultImage\" title=\"Interplay-of-active-processes-modulates-tension-and-drives-phase-transition-in-self-renewing-motor-ncomms10323-s2_ogv\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">Phase transition in self-renewing, motor-driven cytoskeletal networks.<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-354 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:44:16\" data-filename=\"Julia_set_fractal-700x400.png\" data-slide-type=\"image\"><a href=\"https:\/\/commons.wikimedia.org\/wiki\/File:Julia_set_fractal.png\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/Julia_set_fractal-700x400.png\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-354 msDefaultImage\" title=\"Julia_set_fractal\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">Julia Set Fractal. The image is of a colourful computer-generated graphical pattern.<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-356 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:47:37\" data-filename=\"Nematische_Phase_Schlierentextur-601x343.jpg\" data-slide-type=\"image\"><a href=\"https:\/\/commons.wikimedia.org\/w\/index.php?curid=300039\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/Nematische_Phase_Schlierentextur-601x343.jpg\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-356 msDefaultImage\" title=\"Nematische_Phase_Schlierentextur\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">Schlieren texture of liquid crystal nematic phase.<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-358 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:49:40\" data-filename=\"Front_de_percolation-700x400.png\" data-slide-type=\"image\"><a href=\"https:\/\/commons.wikimedia.org\/w\/index.php?curid=1162764\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/Front_de_percolation-700x400.png\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-358 msDefaultImage\" title=\"Front_de_percolation\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">Percolation front on a square lattice at the percolation threshold (59,3%).<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-360 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:50:53\" data-filename=\"Graphene-700x400.jpg\" data-slide-type=\"image\"><a href=\" https:\/\/commons.wikimedia.org\/w\/index.php?curid=11294534\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/Graphene-700x400.jpg\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-360 msDefaultImage\" title=\"Graphene\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">Graphene: an atomic-scale hexagonal lattice made of carbon atoms, an hopping field for electrons.<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-362 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:52:13\" data-filename=\"DLA_Cluster-700x400.jpg\" data-slide-type=\"image\"><a href=\"https:\/\/commons.wikimedia.org\/w\/index.php?curid=794123\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/DLA_Cluster-700x400.jpg\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-362 msDefaultImage\" title=\"OLYMPUS DIGITAL CAMERA\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">A diffusion-limited-aggregation cluster grown from a copper sulfate solution in an electrodeposition cell.<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-364 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:55:01\" data-filename=\"False_color_image_of_the_far_field_of_a_submerged_turbulent_jet-496x283.jpg\" data-slide-type=\"image\"><a href=\"https:\/\/commons.wikimedia.org\/w\/index.php?curid=3082535\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/False_color_image_of_the_far_field_of_a_submerged_turbulent_jet-496x283.jpg\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-364 msDefaultImage\" title=\"False_color_image_of_the_far_field_of_a_submerged_turbulent_jet\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">Visualization by laser-induced fluorescence of a turbulent jet exhibiting a wide range of length scales.<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-366 ms-image \" aria-roledescription=\"slide\" data-date=\"2019-04-05 15:56:27\" data-filename=\"A_tornado_of_fish-700x400.jpg\" data-slide-type=\"image\"><a href=\"https:\/\/commons.wikimedia.org\/w\/index.php?curid=20234085\" target=\"_blank\" aria-label=\"View Slide Details\" class=\"metaslider_image_link\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/web.infn.it\/FRGIM\/wp-content\/uploads\/2019\/04\/A_tornado_of_fish-700x400.jpg\" height=\"400\" width=\"700\" alt=\"\" class=\"slider-342 slide-366 msDefaultImage\" title=\"A_tornado_of_fish\" \/><\/a><div class=\"caption-wrap\"><div class=\"caption\">A big bait ball swirling around a loose kelp stipe. An example of collective animal behavior.<\/div><\/div><\/li>\n            <\/ul>\n        <\/div>\n        \n    <\/div>\n<\/div><\/div>\n\n\n\n<p class=\"has-text-color has-vivid-cyan-blue-color\"><em>Functional and Renormalization Group Methods in Quantum and Statistical Physics<\/em><\/p>\n\n\n\n<p>The project is coordinated by Dr. Gian Paolo Vacca (INFN), and sponsored by ACRI (<a href=\"https:\/\/www.acri.it\/Home\/Index\/2\">Associazione di Fondazioni e Casse di Risparmio Spa<\/a>) under the <em><a href=\"https:\/\/www.acri.it\/PublicFondazioniOnline\/Detail\/4683\">Young Investigator Training Program 2018<\/a><\/em>,  which is intended to foster young international researchers and to promote their scientific collaboration with a network of Italian research institutions.<\/p>\n\n\n\n<p>It includes an opening for short term&nbsp;<strong>individual research fellowships<\/strong> and, related to it, an upcoming&nbsp;<strong>international conference<\/strong>.<\/p>\n\n\n\n<p><em><strong>Scientific framework<\/strong><\/em><\/p>\n\n\n\n<p>Since the seminal work by Wilson and Kadanoff the renormalization group has represented a revolutionary and universal conceptual paradigm. Starting from its early applications to the theory of phase transitions and critical phenomena, it has been by now adopted in a multitude of research areas, for its unifying power and practical convenience. On the other hand, the functional methods, pioneered by Schwinger, Feynman and Dyson, are nowadays considered a reference point and one of the common languages for the community of theoretical physicists. This international project focuses on the latest scientific developments at the interface of functional and renormalization-group methods, and aims at favoring interdisciplinary discussions between communities interested in these two cornerstones of theoretical physics, both at the formal level and at the modern frontiers of their applications. The latter include for instance: the UV completion problem in particle physics and quantum gravity; nonperturbative gauge theories and nuclear physics; out of equilibrium and fluid effective dynamics; strongly correlated fermions in condensed matter; statistical mechanical models; active matter systems; cosmological evolution and astrophysics.<br><\/p>\n\n\n\n<p><strong><em>Scientific and organising committee<\/em><\/strong><br><\/p>\n\n\n\n<table class=\"wp-block-table\"><tbody><tr><\/tr><tr><td>Gian Paolo Vacca<\/td><td>Coordinator<\/td><\/tr><tr><td>Alfio Bonanno<\/td><td>Member<\/td><\/tr><tr><td>Roberto Percacci<\/td><td>Member<\/td><\/tr><tr><td>Andrea Trombettoni<\/td><td>Member<\/td><\/tr><tr><td>Luca Zambelli<\/td><td>Secretary<\/td><\/tr><tr><\/tr><\/tbody><\/table>\n\n\n\n<p><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Functional and Renormalization Group Methods in Quantum and Statistical Physics The project is coordinated by Dr. Gian Paolo Vacca (INFN),<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"open","template":"","meta":{"colormag_page_container_layout":"default_layout","colormag_page_sidebar_layout":"default_layout","footnotes":""},"class_list":["post-2","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/web.infn.it\/FRGIM\/wp-json\/wp\/v2\/pages\/2","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/web.infn.it\/FRGIM\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/web.infn.it\/FRGIM\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/web.infn.it\/FRGIM\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/web.infn.it\/FRGIM\/wp-json\/wp\/v2\/comments?post=2"}],"version-history":[{"count":29,"href":"https:\/\/web.infn.it\/FRGIM\/wp-json\/wp\/v2\/pages\/2\/revisions"}],"predecessor-version":[{"id":570,"href":"https:\/\/web.infn.it\/FRGIM\/wp-json\/wp\/v2\/pages\/2\/revisions\/570"}],"wp:attachment":[{"href":"https:\/\/web.infn.it\/FRGIM\/wp-json\/wp\/v2\/media?parent=2"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}