{"id":41480,"date":"2014-10-30T17:00:00","date_gmt":"2014-10-30T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=1e02f54805f45ce752b721f1c25edbe7"},"modified":"2014-10-30T17:00:00","modified_gmt":"2014-10-30T14:00:00","slug":"lorentz-invariance-in-chiral-kinetic-theory","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=41480","title":{"rendered":"Lorentz Invariance in Chiral Kinetic Theory"},"content":{"rendered":"<p>Author(s): Jing-Yuan Chen, Dam T. Son, Mikhail A. Stephanov, Ho-Ung Yee, and Yi Yin<\/p>\n<p> A kinetic theory, with explicit Lorentz invariance, is derived for chiral fermions in an external electromagnetic field. This theory provides the correct form for the chiral vortical effect \u2014 the appearance of a current in a system undergoing rotation.<\/p>\n<p>[Phys. Rev. Lett. 113, 182302] Published Thu Oct 30, 2014<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): Jing-Yuan Chen, Dam T. Son, Mikhail A. Stephanov, Ho-Ung Yee, and Yi Yin<\/p>\n<p>A kinetic theory, with explicit Lorentz invariance, is derived for chiral fermions in an external electromagnetic field. This theory provides the correct form for the chiral vortical effect &mdash; the appearance of a current in a system undergoing rotation.<\/p>\n<p>[Phys. Rev. Lett. 113, 182302] Published Thu Oct 30, 2014<\/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-41480","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\/41480","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=41480"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/41480\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=41480"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=41480"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=41480"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}