{"id":1347,"date":"2020-12-21T08:55:17","date_gmt":"2020-12-21T08:55:17","guid":{"rendered":"https:\/\/wp.icmm.csic.es\/tqe\/?p=1347"},"modified":"2020-12-21T08:58:14","modified_gmt":"2020-12-21T08:58:14","slug":"nature-review-physics-from-andreev-to-majorana-bound-states-in-hybrid-superconductor-semiconductor-nanowires","status":"publish","type":"post","link":"https:\/\/wp.icmm.csic.es\/tqe\/2020\/12\/21\/nature-review-physics-from-andreev-to-majorana-bound-states-in-hybrid-superconductor-semiconductor-nanowires\/","title":{"rendered":"Nature Review Physics &#8220;From Andreev to Majorana bound states in hybrid superconductor-semiconductor nanowires&#8221;"},"content":{"rendered":"<p>In this <a href=\"https:\/\/www.nature.com\/articles\/s42254-020-0228-y\">review<\/a>, we discuss the main properties of Andreev\u00a0 and Majorana bound states, state-of-the-art techniques for their detection and theoretical progress beyond minimal models, including different types of robust zero modes that may emerge without a band-topological transition.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-medium wp-image-1348\" src=\"https:\/\/wp.icmm.csic.es\/tqe\/wp-content\/uploads\/sites\/23\/2020\/12\/Fig1-300x242.jpg\" alt=\"\" width=\"300\" height=\"242\" srcset=\"https:\/\/wp.icmm.csic.es\/tqe\/wp-content\/uploads\/sites\/23\/2020\/12\/Fig1-300x242.jpg 300w, https:\/\/wp.icmm.csic.es\/tqe\/wp-content\/uploads\/sites\/23\/2020\/12\/Fig1-1024x825.jpg 1024w, https:\/\/wp.icmm.csic.es\/tqe\/wp-content\/uploads\/sites\/23\/2020\/12\/Fig1-768x618.jpg 768w, https:\/\/wp.icmm.csic.es\/tqe\/wp-content\/uploads\/sites\/23\/2020\/12\/Fig1.jpg 1386w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/p>\n","protected":false},"excerpt":{"rendered":"<p>In this review, we discuss the main properties of Andreev\u00a0 and Majorana bound states, state-of-the-art techniques for their detection and theoretical progress beyond minimal models, including different types of robust zero modes that may emerge without a band-topological transition.<\/p>\n","protected":false},"author":56,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"image","meta":{"footnotes":""},"categories":[1],"tags":[17,20,27],"class_list":["post-1347","post","type-post","status-publish","format-image","hentry","category-sin-categoria","tag-majorana","tag-nanowires","tag-topological-superconductivity","post_format-post-format-image"],"_links":{"self":[{"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/posts\/1347","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/users\/56"}],"replies":[{"embeddable":true,"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/comments?post=1347"}],"version-history":[{"count":2,"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/posts\/1347\/revisions"}],"predecessor-version":[{"id":1350,"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/posts\/1347\/revisions\/1350"}],"wp:attachment":[{"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/media?parent=1347"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/categories?post=1347"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/wp.icmm.csic.es\/tqe\/wp-json\/wp\/v2\/tags?post=1347"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}