{"id":66,"date":"2016-03-17T07:38:14","date_gmt":"2016-03-17T14:38:14","guid":{"rendered":"https:\/\/physlabs.colostate.edu\/hep\/?page_id=66"},"modified":"2016-08-15T20:54:58","modified_gmt":"2016-08-16T03:54:58","slug":"sbnicarus","status":"publish","type":"page","link":"https:\/\/physlabs.colostate.edu\/hep\/research\/sbnicarus\/","title":{"rendered":"SBN\/ICARUS"},"content":{"rendered":"<h3>Short-Baseline Neutrino Program at Fermilab<\/h3>\n<p>The Fermilab Short-Baseline Neutrino Program emerged from a joint proposal by three collaborations to use their detectors to perform sensitive searches for \u03bd<sub>e<\/sub> appearance and \u03bd<sub>\u03bc<\/sub> disappearance in the Booster Neutrino Beam. All of the detectors utilize LArTPCs &#8211; liquid argon time projection chambers &#8211; and each contribute to the development of this technology for the <a href=\"http:\/\/www.dunescience.org\/\" target=\"_blank\">long-baseline DUNE experiment<\/a>. The joint scientific goals are outlined in the proposal, available on the <a href=\"http:\/\/arxiv.org\/abs\/1503.01520\" target=\"_blank\">HEP arxiv<\/a>.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-188\" src=\"https:\/\/physlabs.colostate.edu\/hep\/wp-content\/uploads\/sites\/2\/2016\/03\/SBN_Map_Web-300x117.jpg\" alt=\"SBN_Map_Web\" width=\"679\" height=\"265\" srcset=\"https:\/\/physlabs.colostate.edu\/hep\/wp-content\/uploads\/sites\/2\/2016\/03\/SBN_Map_Web-300x117.jpg 300w, https:\/\/physlabs.colostate.edu\/hep\/wp-content\/uploads\/sites\/2\/2016\/03\/SBN_Map_Web-768x299.jpg 768w, https:\/\/physlabs.colostate.edu\/hep\/wp-content\/uploads\/sites\/2\/2016\/03\/SBN_Map_Web-1024x398.jpg 1024w, https:\/\/physlabs.colostate.edu\/hep\/wp-content\/uploads\/sites\/2\/2016\/03\/SBN_Map_Web.jpg 1713w\" sizes=\"auto, (max-width: 679px) 100vw, 679px\" \/><\/p>\n<h3>SBN Far Detector ICARUS T-600<\/h3>\n<p>The CSU group was one of the first US groups to join with the <strong>ICARUS<\/strong> collaboration to bring the world&#8217;s largest liquid argon projection chamber (LAr-TPC) to Fermilab.<\/p>\n<p>The <a href=\"http:\/\/icarus.lngs.infn.it\/\" target=\"_blank\">ICARUS T-600<\/a> detector, comprised of two 300-ton LAr-TPC modules with photodetectors, will serve as the Short-Baseline Program Far Detector, farthest from the BNB primary target. The T-600 is currently being refurbished at CERN following successful operation at the Gran Sasso laboratory from 2010-2014. The T-600 detector will be <a href=\"http:\/\/www.symmetrymagazine.org\/article\/april-2015\/italian-neutrino-experiment-to-move-to-the-us\">moved to Fermilab<\/a> in 2017.<\/p>\n<h3>CSU SBN Group<\/h3>\n<p>Bob Wilson (Professor)<\/p>\n<p>Chris Hilgenberg (PhD student)<\/p>\n<p>Tyler Boone (MS student)<\/p>\n<p>Technical staff:<\/p>\n<p>Dave Warner (Engineer)<\/p>\n<p>Jay Jablonski (Sr. Technician)<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Short-Baseline Neutrino Program at Fermilab The Fermilab Short-Baseline Neutrino Program emerged from a joint proposal by three collaborations to use their detectors to perform sensitive searches for \u03bde appearance and \u03bd\u03bc disappearance in the Booster Neutrino Beam. All of the detectors utilize LArTPCs &#8211; liquid argon time projection chambers &#8211; and each contribute to the &hellip; <\/p>\n<p><a class=\"more-link btn\" href=\"https:\/\/physlabs.colostate.edu\/hep\/research\/sbnicarus\/\">Continue reading<\/a><\/p>\n","protected":false},"author":3,"featured_media":0,"parent":16,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_kad_blocks_custom_css":"","_kad_blocks_head_custom_js":"","_kad_blocks_body_custom_js":"","_kad_blocks_footer_custom_js":"","footnotes":""},"class_list":["post-66","page","type-page","status-publish","hentry","nodate","item-wrap"],"taxonomy_info":[],"featured_image_src_large":false,"author_info":{"display_name":"buchanan","author_link":"https:\/\/physlabs.colostate.edu\/hep\/author\/buchanan\/"},"comment_info":0,"_links":{"self":[{"href":"https:\/\/physlabs.colostate.edu\/hep\/wp-json\/wp\/v2\/pages\/66","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/physlabs.colostate.edu\/hep\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/physlabs.colostate.edu\/hep\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/physlabs.colostate.edu\/hep\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/physlabs.colostate.edu\/hep\/wp-json\/wp\/v2\/comments?post=66"}],"version-history":[{"count":5,"href":"https:\/\/physlabs.colostate.edu\/hep\/wp-json\/wp\/v2\/pages\/66\/revisions"}],"predecessor-version":[{"id":194,"href":"https:\/\/physlabs.colostate.edu\/hep\/wp-json\/wp\/v2\/pages\/66\/revisions\/194"}],"up":[{"embeddable":true,"href":"https:\/\/physlabs.colostate.edu\/hep\/wp-json\/wp\/v2\/pages\/16"}],"wp:attachment":[{"href":"https:\/\/physlabs.colostate.edu\/hep\/wp-json\/wp\/v2\/media?parent=66"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}