{"id":9871,"date":"2023-09-06T15:52:13","date_gmt":"2023-09-06T13:52:13","guid":{"rendered":"https:\/\/www.dm.unipi.it\/?post_type=unipievents&#038;p=9871"},"modified":"2023-09-06T15:52:15","modified_gmt":"2023-09-06T13:52:15","slug":"homogeneous-and-heterogeneous-nucleation-in-the-three-state-blume-capel-model","status":"publish","type":"unipievents","link":"https:\/\/www.dm.unipi.it\/en\/eventi\/homogeneous-and-heterogeneous-nucleation-in-the-three-state-blume-capel-model\/","title":{"rendered":"Homogeneous and heterogeneous nucleation in the three-state Blume-Capel model &ndash; Vanessa Jacquier (University of Utrecht)"},"content":{"rendered":"\n<p>We study the metastable behavior of the stochastic Blume\u2013Capel model evolving according to the Glauber dynamics with zero boundary conditions. We will show that, due to the three\u2013state character of the Blume\u2013Capel model, the metastability scenario proven for periodic boundary conditions changes deeply when different boundary conditions are considered. The Hamiltonian of the Blume\u2013Capel model depends on the magnetic field h and the chemical potential \u03bb. We study the heuristic in the whole region \u03bb,h &gt; 0, where the chemical potential term equally favors minus and plus spins with respect to zeroes and the magnetic field favors pluses and disadvantages minuses with respect to the zeroes, and we compare our results with the Blume-Capel model with periodic boundary conditions. Then, we analyze in detail the region \u03bb&gt;h &gt; 0. In this region, we identify the unique metastable state -1, we compute the energy barrier from -1 to the stable state +1, and we find an estimate for the asymptotic behavior of the transition time from the metastable to the stable state as \u03b2-&gt;\u221e, where \u03b2 is the inverse of the temperature.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>We study the metastable behavior of the stochastic Blume\u2013Capel model evolving according to the Glauber dynamics with zero boundary conditions.&hellip;<\/p>\n<p><a class=\"btn btn-dark btn-sm unipi-read-more-link\" href=\"https:\/\/www.dm.unipi.it\/en\/eventi\/homogeneous-and-heterogeneous-nucleation-in-the-three-state-blume-capel-model\/\">Read More&#8230;<\/a><\/p>\n","protected":false},"author":105,"featured_media":0,"template":"","tags":[],"unipievents_taxonomy":[],"class_list":["post-9871","unipievents","type-unipievents","status-publish","hentry"],"acf":[],"unipievents_startdate":1694530800,"unipievents_enddate":1694534400,"unipievents_place":"Aula Seminari","unipievents_externalid":0,"jetpack_sharing_enabled":true,"publishpress_future_workflow_manual_trigger":{"enabledWorkflows":[]},"_links":{"self":[{"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/unipievents\/9871","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/unipievents"}],"about":[{"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/types\/unipievents"}],"author":[{"embeddable":true,"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/users\/105"}],"version-history":[{"count":2,"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/unipievents\/9871\/revisions"}],"predecessor-version":[{"id":9873,"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/unipievents\/9871\/revisions\/9873"}],"wp:attachment":[{"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/media?parent=9871"}],"wp:term":[{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/tags?post=9871"},{"taxonomy":"unipievents_taxonomy","embeddable":true,"href":"https:\/\/www.dm.unipi.it\/en\/wp-json\/wp\/v2\/unipievents_taxonomy?post=9871"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}