{"id":10876,"date":"2022-06-06T12:41:00","date_gmt":"2022-06-06T10:41:00","guid":{"rendered":"https:\/\/www.pi.infn.it\/?p=10876"},"modified":"2022-06-13T14:18:53","modified_gmt":"2022-06-13T12:18:53","slug":"one-dimensional-qcd-oleg-borisenko-n-n-bogolyubov-insitute-for-theoretical-physics-national-academy-of-sciences-of-ukraine-kyiv","status":"publish","type":"post","link":"https:\/\/www.pi.infn.it\/?p=10876","title":{"rendered":"One-dimensional QCD (Oleg Borisenko, N.N. Bogolyubov Insitute for Theoretical Physics, National Academy of Sciences of Ukraine, Kyiv)"},"content":{"rendered":"\n<div class=\"myutilsext\"><p class=\"abstract\" style=\"text-align: justify\"><br \/>ABSTRACT: I review exact solutions of the one-dimensional QCD at finite temperature and non-zero chemical potential for the gauge groups G=Z(N),U(N),SU(N) for all values of colors N and fermion flavors N_f. Such solutions are available both for the partition function and various expectation values. The phase structure in the large N, the large N_f and the &#8216;t Hooft-Veneziano limits of all models is also discussed. A comparision of all limits with SU(3) QCD and with free fermion model is performed.<\/p>\n<p>Il seminario si terr\u00e0 in modalit\u00e0 remota sulla piattaforma\u00a0 Zoom al seguente indirizzo:<\/p>\n<p><a class=\"moz-txt-link-freetext\" href=\"https:\/\/infn-it.zoom.us\/j\/84261721878?pwd=MDZNaGdBUlcvUUJXa2phSHZVZk5sdz09\">https:\/\/infn-it.zoom.us\/j\/84261721878?pwd=MDZNaGdBUlcvUUJXa2phSHZVZk5sdz09<\/a><br \/><br \/>ID riunione: 842 6172 1878<br \/>Passcode: 611379<\/p>\n<p>Le slides sono caricate su:<\/p>\n<p><a href=\"https:\/\/agenda.infn.it\/event\/31495\/\">https:\/\/agenda.infn.it\/event\/31495\/<\/a><\/p>\n<p>\u00a0<\/p><\/div>\n\n\n\n<p><\/p>\n\n\n<figure class=\"wp-block-post-featured-image\"><img width=\"1388\" height=\"805\" src=\"https:\/\/www.pi.infn.it\/wp-content\/uploads\/2022\/06\/Seminario-Borisenko.jpg\" class=\"attachment-post-thumbnail size-post-thumbnail wp-post-image\" alt=\"\" decoding=\"async\" loading=\"lazy\" srcset=\"https:\/\/www.pi.infn.it\/wp-content\/uploads\/2022\/06\/Seminario-Borisenko.jpg 1388w, https:\/\/www.pi.infn.it\/wp-content\/uploads\/2022\/06\/Seminario-Borisenko-300x174.jpg 300w, https:\/\/www.pi.infn.it\/wp-content\/uploads\/2022\/06\/Seminario-Borisenko-1024x594.jpg 1024w, https:\/\/www.pi.infn.it\/wp-content\/uploads\/2022\/06\/Seminario-Borisenko-768x445.jpg 768w\" sizes=\"(max-width: 1388px) 100vw, 1388px\" \/><\/figure>\n\n","protected":false},"excerpt":{"rendered":"<p>ABSTRACT: I review exact solutions of the one-dimensional QCD at finite temperature and non-zero chemical potential for the gauge groups G=Z(N),U(N),SU(N) for all values of colors N and fermion flavors N_f. Such solutions are available both for the partition function and various expectation values. The phase structure in the large N, the large N_f and the &#8216;t Hooft-Veneziano limits of all models is also discussed. A comparision of all limits with SU(3) QCD and with free fermion model is performed.<\/p>\n","protected":false},"author":26,"featured_media":10877,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_links_to":"","_links_to_target":""},"categories":[8],"tags":[],"publishpress_future_action":{"enabled":false,"date":"2026-05-13 19:37:12","action":"change-status","newStatus":"draft","terms":[],"taxonomy":"category"},"_links":{"self":[{"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=\/wp\/v2\/posts\/10876"}],"collection":[{"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=\/wp\/v2\/users\/26"}],"replies":[{"embeddable":true,"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=10876"}],"version-history":[{"count":10,"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=\/wp\/v2\/posts\/10876\/revisions"}],"predecessor-version":[{"id":10947,"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=\/wp\/v2\/posts\/10876\/revisions\/10947"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=\/wp\/v2\/media\/10877"}],"wp:attachment":[{"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=10876"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=10876"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.pi.infn.it\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=10876"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}