{"id":304192,"date":"2016-10-19T17:00:00","date_gmt":"2016-10-19T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=dbfda9d1aba16a1b839679e2fa3a559f"},"modified":"2016-10-19T17:00:00","modified_gmt":"2016-10-19T14:00:00","slug":"direct-observation-of-a-long-range-field-effect-from-gate-tuning-of-nonlocal-conductivity","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=304192","title":{"rendered":"Direct Observation of a Long-Range Field Effect from Gate Tuning of Nonlocal Conductivity"},"content":{"rendered":"<p>Author(s): Lin Wang, Ignacio Guti\u00e9rrez-Lezama, C\u00e9line Barreteau, Dong-Keun Ki, Enrico Giannini, and Alberto F. Morpurgo<\/p>\n<p>An unconventional long-range field effect in WTe<math xmlns=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\"><msub><mrow><\/mrow><mn>2<\/mn><\/msub><\/math> is used to gate-tune the bulk properties of the material. This method could be used to gate-tune electronic properties deep in the interior of conducting materials, avoiding limitations imposed by electrostatic screening.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.117.176601.png\" width=\"200\" height=\"100\"><\/p>\n<p>[Phys. Rev. Lett. 117, 176601] Published Wed Oct 19, 2016<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): Lin Wang, Ignacio Guti&eacute;rrez-Lezama, C&eacute;line Barreteau, Dong-Keun Ki, Enrico Giannini, and Alberto F. Morpurgo<\/p>\n<p>An unconventional long-range field effect in WTe2 is used to gate-tune the bulk properties of the material. This method could be used to gate-tune electronic properties deep in the interior of conducting materials, avoiding limitations imposed by electrostatic screening.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.117.176601.png\" width=\"200\" height='\"100\"'><br \/>[Phys. Rev. Lett. 117, 176601] Published Wed Oct 19, 2016<\/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-304192","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\/304192","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=304192"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/304192\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=304192"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=304192"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=304192"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}