{"id":895,"date":"2014-03-03T11:32:26","date_gmt":"2014-03-03T02:32:26","guid":{"rendered":"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/"},"modified":"2014-03-03T11:32:26","modified_gmt":"2014-03-03T02:32:26","slug":"phase_structure_study_of_su2_lattice_gauge_theory_with_8_flavours","status":"publish","type":"seminar","link":"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/","title":{"rendered":"Phase structure study of SU(2) lattice gauge theory with 8 flavours"},"content":{"rendered":"<p><span>In this talk, I would like to present the phase structure of SU(2) lattice gauge theory&nbsp;<\/span><span>with 8 flavours(staggered fermions) in fundamental representation.&nbsp;<\/span><span>Average plaquette and Polyakov loop are measured and one phase transition is observed.&nbsp;<\/span><span>To identify the order of this confining-deconfining phase transition,&nbsp;<\/span><span>we resort to the study of cold &amp; hot-start simulations for plaquette.&nbsp;<\/span><span>Moreover, studies of APE smearing, autocorrelation time, effective potential,&nbsp;<\/span><span>and susceptibility are further done for Polyakov loop.&nbsp;<\/span><span>Finally, I would show results of some zero mass simulations&nbsp;<\/span><span>as a starting point to study the chiral condensate,&nbsp;<\/span><span>being the order parameter for spontaneous chiral symmetry breaking.&nbsp;<\/span><span>Moreover, some future works will be mentioned.<\/span><\/p>\n<div><span><br \/><\/span><\/div>\n","protected":false},"featured_media":0,"template":"","tags":[],"seminar_category":[53],"acf":{"s_now_accepting":true,"s_date_order":"2014-02-21 13:30:00","s_date_end":null,"s_date_text":"","s_text":"Cynthia Yu-Han Huang","s_place":"KMI Science Symposia (ES635)","s_place_other":"","s_categoryother":"KMI Theory Informal Seminar","s_poster":"","s_poster2":"","s_slide":""},"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v23.5 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>Phase structure study of SU(2) lattice gauge theory with 8 flavours - KMI - Nagoya University<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Phase structure study of SU(2) lattice gauge theory with 8 flavours - KMI - Nagoya University\" \/>\n<meta property=\"og:description\" content=\"In this talk, I would like to present the phase structure of SU(2) lattice gauge theory&nbsp;with 8 flavours(staggered fermions) in fundamental representation.&nbsp;Average plaquette and Polyakov loop are measured and one phase transition is observed.&nbsp;To identify the order of this confining-deconfining phase transition,&nbsp;we resort to the study of cold &amp; hot-start simulations for plaquette.&nbsp;Moreover, studies of APE smearing, autocorrelation time, effective potential,&nbsp;and susceptibility are further done for Polyakov loop.&nbsp;Finally, I would show results of some zero mass simulations&nbsp;as a starting point &hellip;\" \/>\n<meta property=\"og:url\" content=\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/\" \/>\n<meta property=\"og:site_name\" content=\"KMI - Nagoya University\" \/>\n<meta name=\"twitter:card\" content=\"summary_large_image\" \/>\n<meta name=\"twitter:label1\" content=\"Est. reading time\" \/>\n\t<meta name=\"twitter:data1\" content=\"1 minute\" \/>\n<script type=\"application\/ld+json\" class=\"yoast-schema-graph\">{\"@context\":\"https:\/\/schema.org\",\"@graph\":[{\"@type\":\"WebPage\",\"@id\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/\",\"url\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/\",\"name\":\"Phase structure study of SU(2) lattice gauge theory with 8 flavours - KMI - Nagoya University\",\"isPartOf\":{\"@id\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/#website\"},\"datePublished\":\"2014-03-03T02:32:26+00:00\",\"dateModified\":\"2014-03-03T02:32:26+00:00\",\"breadcrumb\":{\"@id\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/#breadcrumb\"},\"inLanguage\":\"en-US\",\"potentialAction\":[{\"@type\":\"ReadAction\",\"target\":[\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/\"]}]},{\"@type\":\"BreadcrumbList\",\"@id\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/#breadcrumb\",\"itemListElement\":[{\"@type\":\"ListItem\",\"position\":1,\"name\":\"Home\",\"item\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/\"},{\"@type\":\"ListItem\",\"position\":2,\"name\":\"Seminars\",\"item\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/\"},{\"@type\":\"ListItem\",\"position\":3,\"name\":\"Phase structure study of SU(2) lattice gauge theory with 8 flavours\"}]},{\"@type\":\"WebSite\",\"@id\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/#website\",\"url\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/\",\"name\":\"KMI - Nagoya University\",\"description\":\"Nagoya University: Kobayashi-Maskawa Institute for the Origin of Particles and the Universe (KMI)\",\"potentialAction\":[{\"@type\":\"SearchAction\",\"target\":{\"@type\":\"EntryPoint\",\"urlTemplate\":\"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/?s={search_term_string}\"},\"query-input\":{\"@type\":\"PropertyValueSpecification\",\"valueRequired\":true,\"valueName\":\"search_term_string\"}}],\"inLanguage\":\"en-US\"}]}<\/script>\n<!-- \/ Yoast SEO plugin. -->","yoast_head_json":{"title":"Phase structure study of SU(2) lattice gauge theory with 8 flavours - KMI - Nagoya University","robots":{"index":"index","follow":"follow","max-snippet":"max-snippet:-1","max-image-preview":"max-image-preview:large","max-video-preview":"max-video-preview:-1"},"canonical":"https:\/\/www.kmi.nagoya-u.ac.jp\/eng\/seminar\/895\/","og_locale":"en_US","og_type":"article","og_title":"Phase structure study of SU(2) lattice gauge theory with 8 flavours - KMI - Nagoya University","og_description":"In this talk, I would like to present the phase structure of SU(2) lattice gauge theory&nbsp;with 8 flavours(staggered fermions) in fundamental representation.&nbsp;Average plaquette and Polyakov loop are measured and one phase transition is observed.&nbsp;To identify the order of this confining-deconfining phase transition,&nbsp;we resort to the study of cold &amp; 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