{"id":2801,"date":"2021-04-23T18:21:32","date_gmt":"2021-04-23T09:21:32","guid":{"rendered":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/?p=2801"},"modified":"2021-04-23T18:34:58","modified_gmt":"2021-04-23T09:34:58","slug":"giant-orbital-diamagnetism-of-three-dimensional-dirac-electrons-in-sr3pbo-antiperovskite","status":"publish","type":"post","link":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/news\/2801\/","title":{"rendered":"Giant orbital diamagnetism of three-dimensional Dirac electrons in&nbsp;Sr3PbO&nbsp;antiperovskite"},"content":{"rendered":"\n<div class=\"wp-block-image\"><figure class=\"alignright size-full is-resized\"><a href=\"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-content\/uploads\/sites\/2\/2021\/04\/press20210423-1.jpg\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-content\/uploads\/sites\/2\/2021\/04\/press20210423-1.jpg\" alt=\"\" class=\"wp-image-2810\" width=\"640\" height=\"277\" srcset=\"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-content\/uploads\/sites\/2\/2021\/04\/press20210423-1.jpg 1280w, https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-content\/uploads\/sites\/2\/2021\/04\/press20210423-1-300x130.jpg 300w, https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-content\/uploads\/sites\/2\/2021\/04\/press20210423-1-1024x443.jpg 1024w\" sizes=\"(max-width: 640px) 100vw, 640px\" \/><\/a><\/figure><\/div>\n\n\n\n<p>In Dirac semimetals, interband mixing has been known theoretically to give rise to a giant orbital diamagnetism when the Fermi level is close to the Dirac point. In&nbsp;Bi<sub>1\u2212x<\/sub>Sb<sub>x<\/sub>&nbsp;and other Dirac semimetals, an enhanced diamagnetism in the magnetic susceptibility&nbsp;<em>\u03c7<\/em>&nbsp;has been observed and interpreted as a manifestation of such giant orbital diamagnetism. Experimentally proving their orbital origin, however, has remained challenging. The cubic antiperovskite&nbsp;Sr<sub>3<\/sub>PbO&nbsp;is a three-dimensional Dirac electron system and shows the giant diamagnetism in&nbsp;<em>\u03c7<\/em>&nbsp;as in the other Dirac semimetals.&nbsp;<sup>207<\/sup>Pb&nbsp;NMR measurements are conducted in this study to explore the microscopic origin of diamagnetism. From the analysis of the Knight shift&nbsp;<em>K<\/em>&nbsp;as a function of&nbsp;<em>\u03c7&nbsp;<\/em>&nbsp;and the relaxation rate&nbsp;<em>T<sub>1<\/sub><sup>\u20131<\/sup><\/em>&nbsp;for samples with different hole densities, the spin and the orbital components in&nbsp;<em>K<\/em>&nbsp;are successfully separated. The results establish that the enhanced diamagnetism in&nbsp;Sr<sub>3<\/sub>PbO&nbsp;originates from the orbital contribution of Dirac electrons, which is fully consistent with the theory of giant orbital diamagnetism.<\/p>\n\n\n\n<p>See below for more information.<\/p>\n\n\n\n<ul><li>Aritcle URL :\u00a0<a href=\"https:\/\/journals.aps.org\/prb\/abstract\/10.1103\/PhysRevB.103.115117\" data-type=\"URL\" data-id=\"https:\/\/journals.aps.org\/prb\/abstract\/10.1103\/PhysRevB.103.115117\">https:\/\/journals.aps.org\/prb\/abstract\/10.1103\/PhysRevB.103.115117<\/a><\/li><li>Takagi-Kitagawa Lab. :\u00a0<a href=\"http:\/\/park.itc.u-tokyo.ac.jp\/takagi_lab\/en\/\">http:\/\/park.itc.u-tokyo.ac.jp\/takagi_lab\/en\/<\/a><\/li><li>Ogata Lab. : <a href=\"https:\/\/sites.google.com\/hosi.phys.s.u-tokyo.ac.jp\/homepage\/english\">https:\/\/sites.google.com\/hosi.phys.s.u-tokyo.ac.jp\/homepage\/english<\/a><\/li><\/ul>\n\n\n","protected":false},"excerpt":{"rendered":"In Dirac semimetals, interband mixing has been known theoretically to give rise to a giant orbital diamagnetis [&hellip;]","protected":false},"author":7,"featured_media":2810,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":[],"categories":[3],"tags":[11,36,10],"_links":{"self":[{"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/posts\/2801"}],"collection":[{"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/users\/7"}],"replies":[{"embeddable":true,"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/comments?post=2801"}],"version-history":[{"count":9,"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/posts\/2801\/revisions"}],"predecessor-version":[{"id":2812,"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/posts\/2801\/revisions\/2812"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/media\/2810"}],"wp:attachment":[{"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/media?parent=2801"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/categories?post=2801"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.phys.s.u-tokyo.ac.jp\/en\/wp-json\/wp\/v2\/tags?post=2801"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}