{"id":4549,"date":"2024-03-27T14:59:10","date_gmt":"2024-03-27T14:59:10","guid":{"rendered":"https:\/\/iap.um6p.ma\/?p=4549"},"modified":"2024-03-30T20:27:03","modified_gmt":"2024-03-30T20:27:03","slug":"4549","status":"publish","type":"post","link":"https:\/\/physicsschool.um6p.ma\/?p=4549","title":{"rendered":"New Research Article"},"content":{"rendered":"<p>Check out our new article on <span style=\"color: #000080;\"><em><strong>Graphene quantum dot bolometer for on-chip detection of organic radical<\/strong><\/em><\/span>.<br \/>\nRead the full letter here: <span style=\"text-decoration: underline; color: #0000ff;\"><a style=\"color: #0000ff; text-decoration: underline;\" href=\"https:\/\/pubs.aip.org\/aip\/apl\/article\/124\/12\/123505\/3278020\/\">https:\/\/pubs.aip.org\/aip\/apl\/article\/124\/12\/123505\/3278020\/<\/a><\/span><\/p>\n<p><strong><span style=\"text-decoration: underline;\">Abstract<\/span><\/strong><\/p>\n<p>We present a proof-of-concept magnetic resonance detection of organic radical 2,2-diphenyl-1-picrylhydrazyl via a nanostructured on-chip graphene quantum dot bolometer. In a common electron paramagnetic resonance setup, the microwave propagates from a source into a sample and back to a detector. Yet, by using on-chip detection, it is possible to skip the whole detection arm and, thus, mitigate lab expenses on instrument and cooling costs. The bolometric detection was demonstrated at a frequency of 151\u2009GHz and a temperature of 15\u2009K.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Check out our new article on Graphene quantum dot bolometer for on-chip detection of organic radical. Read the full letter here: https:\/\/pubs.aip.org\/aip\/apl\/article\/124\/12\/123505\/3278020\/ Abstract We present a proof-of-concept magnetic resonance detection of organic radical 2,2-diphenyl-1-picrylhydrazyl via a nanostructured on-chip graphene quantum dot bolometer. In a common electron paramagnetic resonance setup, the microwave propagates from a source [&hellip;]<\/p>\n","protected":false},"author":3,"featured_media":4558,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"cybocfi_hide_featured_image":"yes","footnotes":""},"categories":[1],"tags":[],"class_list":["post-4549","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-uncategorized"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=\/wp\/v2\/posts\/4549","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=4549"}],"version-history":[{"count":10,"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=\/wp\/v2\/posts\/4549\/revisions"}],"predecessor-version":[{"id":4586,"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=\/wp\/v2\/posts\/4549\/revisions\/4586"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=\/wp\/v2\/media\/4558"}],"wp:attachment":[{"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=4549"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=4549"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/physicsschool.um6p.ma\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=4549"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}