{"id":15,"date":"2014-05-12T07:51:52","date_gmt":"2014-05-12T05:51:52","guid":{"rendered":"http:\/\/phsites.technion.ac.il\/dtqm\/?p=15"},"modified":"2014-05-14T14:37:53","modified_gmt":"2014-05-14T12:37:53","slug":"duncan-haldane-3d-topological-metals-2d-surface-fermi-arcs-cancelation-chiral-magnetic-effect","status":"publish","type":"post","link":"https:\/\/phsites.technion.ac.il\/dtqm\/duncan-haldane-3d-topological-metals-2d-surface-fermi-arcs-cancelation-chiral-magnetic-effect\/","title":{"rendered":"3D Topological metals, 2D surface Fermi arcs and cancelation of the chiral magnetic effect."},"content":{"rendered":"<h2>Duncan Haldane<\/h2>\n<p>When the Fermi-liquid description is applied to 3D metals with \u00a0multiple disjoint Fermi surface sheets, it becomes apparent that metallic Fermi-liquids can be classified as \u00a0&#8220;Symmetry-Protected Topological (SPT) states&#8221;, which in general support a separate quasiparticle current associated with each disjoint \u00a0sheet. An exception occurs when \u00a0the quasiparticle states on a sheet define a &#8220;U(1) fiber bundle&#8221; with non-vanishing first Chern class (&#8220;Chern number&#8221;), so its current conservation law exhibits a chiral anomaly, which apparently leads to a &#8220;chiral magnetic effecr&#8221; (CME) when an applied \u00a0electric field has a component parallel to an applied magnetic flux density. However, such Fermi surfaces are always connected into groups with \u00a0vanishing total Chern number by \u00a0surface Fermi arcs, first discovered in studies of Weyl semimetals, but which are a general feature of topologcally-non-trivial Fermi surfaces. \u00a0\u00a0The 2D surface Fermi arcs cancel the bulk CME, and maintain a common chemical potential on the bulk 3D \u00a0Fermi-surface sheets that they connect. \u00a0\u00a0\u00a0The surface Fermi arcs are supported by non-standard surface states of &#8220;Shockley type&#8221; that do not form complete bands in the surface Brillouin zone, which is a generic feature of\u00a0 topological surface states.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Duncan Haldane When the Fermi-liquid description is applied to 3D metals with \u00a0multiple disjoint Fermi surface sheets, it becomes apparent that metallic Fermi-liquids can be classified as \u00a0&#8220;Symmetry-Protected Topological (SPT) states&#8221;, which in general support a separate quasiparticle current associated with each disjoint \u00a0sheet. An exception occurs when \u00a0the quasiparticle states on a sheet define &hellip;<\/p>\n","protected":false},"author":2,"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":[1],"tags":[],"class_list":{"0":"post-15","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-uncategorized","7":"entry"},"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.6 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>3D Topological metals, 2D surface Fermi arcs and cancelation of the chiral magnetic effect. - Dynamics and Transport in Quantum Matter<\/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:\/\/phsites.technion.ac.il\/dtqm\/duncan-haldane-3d-topological-metals-2d-surface-fermi-arcs-cancelation-chiral-magnetic-effect\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"3D Topological metals, 2D surface Fermi arcs and cancelation of the chiral magnetic effect. - Dynamics and Transport in Quantum Matter\" \/>\n<meta property=\"og:description\" content=\"Duncan Haldane When the Fermi-liquid description is applied to 3D metals with \u00a0multiple disjoint Fermi surface sheets, it becomes apparent that metallic Fermi-liquids can be classified as \u00a0&#8220;Symmetry-Protected Topological (SPT) states&#8221;, which in general support a separate quasiparticle current associated with each disjoint \u00a0sheet. An exception occurs when \u00a0the quasiparticle states on a sheet define &hellip;\" \/>\n<meta property=\"og:url\" content=\"https:\/\/phsites.technion.ac.il\/dtqm\/duncan-haldane-3d-topological-metals-2d-surface-fermi-arcs-cancelation-chiral-magnetic-effect\/\" \/>\n<meta property=\"og:site_name\" content=\"Dynamics and Transport in Quantum Matter\" \/>\n<meta property=\"article:published_time\" content=\"2014-05-12T05:51:52+00:00\" \/>\n<meta property=\"article:modified_time\" content=\"2014-05-14T12:37:53+00:00\" \/>\n<meta name=\"author\" content=\"Adi\" \/>\n<meta name=\"twitter:label1\" content=\"Written by\" \/>\n\t<meta name=\"twitter:data1\" content=\"Adi\" \/>\n\t<meta name=\"twitter:label2\" content=\"Est. reading time\" \/>\n\t<meta name=\"twitter:data2\" content=\"1 minute\" \/>\n<script type=\"application\/ld+json\" class=\"yoast-schema-graph\">{\"@context\":\"https:\\\/\\\/schema.org\",\"@graph\":[{\"@type\":\"Article\",\"@id\":\"https:\\\/\\\/phsites.technion.ac.il\\\/dtqm\\\/duncan-haldane-3d-topological-metals-2d-surface-fermi-arcs-cancelation-chiral-magnetic-effect\\\/#article\",\"isPartOf\":{\"@id\":\"https:\\\/\\\/phsites.technion.ac.il\\\/dtqm\\\/duncan-haldane-3d-topological-metals-2d-surface-fermi-arcs-cancelation-chiral-magnetic-effect\\\/\"},\"author\":{\"name\":\"Adi\",\"@id\":\"https:\\\/\\\/phsites.technion.ac.il\\\/dtqm\\\/#\\\/schema\\\/person\\\/65231d9f0ecb94f8411926c66a3791ff\"},\"headline\":\"3D Topological metals, 2D surface Fermi arcs and cancelation of the chiral magnetic effect.\",\"datePublished\":\"2014-05-12T05:51:52+00:00\",\"dateModified\":\"2014-05-14T12:37:53+00:00\",\"mainEntityOfPage\":{\"@id\":\"https:\\\/\\\/phsites.technion.ac.il\\\/dtqm\\\/duncan-haldane-3d-topological-metals-2d-surface-fermi-arcs-cancelation-chiral-magnetic-effect\\\/\"},\"wordCount\":205,\"inLanguage\":\"en-US\"},{\"@type\":\"WebPage\",\"@id\":\"https:\\\/\\\/phsites.technion.ac.il\\\/dtqm\\\/duncan-haldane-3d-topological-metals-2d-surface-fermi-arcs-cancelation-chiral-magnetic-effect\\\/\",\"url\":\"https:\\\/\\\/phsites.technion.ac.il\\\/dtqm\\\/duncan-haldane-3d-topological-metals-2d-surface-fermi-arcs-cancelation-chiral-magnetic-effect\\\/\",\"name\":\"3D Topological metals, 2D surface Fermi arcs and cancelation of the chiral magnetic effect. - 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