{"id":424971,"date":"2017-06-23T17:00:00","date_gmt":"2017-06-23T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=e6afea3c66898a415ee0520cf730feb2"},"modified":"2017-06-23T17:00:00","modified_gmt":"2017-06-23T14:00:00","slug":"controlling-the-topological-sector-of-magnetic-solitons-in-exfoliated-cr_13-nbs_2-crystals","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=424971","title":{"rendered":"Controlling the Topological Sector of Magnetic Solitons in Exfoliated Cr_{1\/3} NbS_{2} Crystals"},"content":{"rendered":"<p>Author(s): L. Wang, N. Chepiga, D.-K. Ki, L. Li, F. Li, W. Zhu, Y. Kato, O.\u2009S. Ovchinnikova, F. Mila, I. Martin, D. Mandrus, and A.\u2009F. Morpurgo<\/p>\n<p>Film thickness dependent changes in the topological properties of magnetic solitons are tracked via magnetotransport measurements in exfoliated crystals of the monoaxial chiral helimagnet Cr<math xmlns=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\"><msub><mrow><\/mrow><mrow><mn>1<\/mn><mo stretchy=\"false\" rspace=\"0\" lspace=\"0\">\/<\/mo><mn>3<\/mn><\/mrow><\/msub><\/math>NbS<math xmlns=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\"><msub><mrow><\/mrow><mn>2<\/mn><\/msub><\/math>.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.118.257203.png\" width=\"200\" height=\\\"100\\\"><\/p>\n<p>[Phys. Rev. Lett. 118, 257203] Published Fri Jun 23, 2017<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): L. Wang, N. Chepiga, D.-K. Ki, L. Li, F. Li, W. Zhu, Y. Kato, O.&thinsp;S. Ovchinnikova, F. Mila, I. Martin, D. Mandrus, and A.&thinsp;F. Morpurgo<\/p>\n<p>Film thickness dependent changes in the topological properties of magnetic solitons are tracked via magnetotransport measurements in exfoliated crystals of the monoaxial chiral helimagnet Cr1\/3NbS2.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.118.257203.png\" width=\"200\" height='\"100\"'><br \/>[Phys. Rev. Lett. 118, 257203] Published Fri Jun 23, 2017<\/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-424971","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\/424971","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=424971"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/424971\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=424971"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=424971"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=424971"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}