{"id":435851,"date":"2017-07-25T17:00:00","date_gmt":"2017-07-25T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=a2d2567a8f3076d73787859fa2265449"},"modified":"2017-07-25T17:00:00","modified_gmt":"2017-07-25T14:00:00","slug":"determinant-diagrammatic-monte-carlo-algorithm-in-the-thermodynamic-limit","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=435851","title":{"rendered":"Determinant Diagrammatic Monte\u00a0Carlo Algorithm in the Thermodynamic Limit"},"content":{"rendered":"<p>Author(s): Riccardo Rossi<\/p>\n<p>High-order diagrammatic expansions for fermionic systems can be computed by considering the sum of all connected Feynman diagrams at fixed positions of interaction vertices. The method is an improvement over conventional diagrammatic Monte Carlo computations.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.119.045701.png\" width=\"200\" height=\\\"100\\\"><\/p>\n<p>[Phys. Rev. Lett. 119, 045701] Published Tue Jul 25, 2017<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): Riccardo RossiHigh-order diagrammatic expansions for fermionic systems can be computed by considering the sum of all connected Feynman diagrams at fixed positions of interaction vertices. The method is an improvement over conventional diagra&#8230;<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_genesis_hide_title":false,"_genesis_hide_breadcrumbs":false,"_genesis_hide_singular_image":false,"_genesis_hide_footer_widgets":false,"_genesis_custom_body_class":"","_genesis_custom_post_class":"","_genesis_layout":"","footnotes":""},"categories":[182],"tags":[],"class_list":{"0":"post-435851","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-rss-teadus","7":"entry"},"_links":{"self":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/435851","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=435851"}],"version-history":[{"count":1,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/435851\/revisions"}],"predecessor-version":[{"id":503924,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/435851\/revisions\/503924"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=435851"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=435851"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=435851"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}