{"id":7777,"date":"2022-01-11T10:02:52","date_gmt":"2022-01-11T10:02:52","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=7777"},"modified":"2022-06-21T09:53:31","modified_gmt":"2022-06-21T09:53:31","slug":"silicon-carbide-characterization-at-the-n_tof-spallation-source-with-quasi-monoenergetic-fast-neutrons","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/silicon-carbide-characterization-at-the-n_tof-spallation-source-with-quasi-monoenergetic-fast-neutrons\/","title":{"rendered":"Silicon Carbide characterization at the n_TOF spallation source with quasi-monoenergetic fast neutrons"},"content":{"rendered":"<p>Silicon Carbide (SiC) is a relatively new entry in the world of solid-state detectors. Although SiC response to neutrons is more complex than the one obtained with diamonds, the measured energy resolution (FWHM\/E-d <4%) makes SiC an interesting alternative to diamond and silicon detectors for fast neutrons. The results obtained from the measurements of the response of a 100 um thick SiC detector to neutrons in the energy range between 3 and 20 MeV at the n_TOF spallation source at CERN are presented in this paper. By selecting the neutron energy by means of the time of flight, the detector response to quasi-mono-energetic neutrons was measured. The main neutron-induced nuclear reactions were identified in the measured pulse height spectrum. Detection efficiency as a function of neutron energy was measured and interpreted based on available neutron cross section and by making use of Monte Carlo simulations.\n<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Kushoro, M. H.; Rebai, M.; Dicorato, M.; Rigamonti, D.; Altana, C.; Cazzaniga, C.; Croci, G.; Gorini, G.; Lanzalone, G.; La Via, F.; Muoio, A.; Muraro, A.; Murtas, F.; Cippo, E. Perelli; Tardocchi, M.; Barbagallo, M.; Mingrone, F.; Tudisco, S.<\/p>\n","protected":false},"featured_media":1294,"comment_status":"closed","ping_status":"open","template":"","meta":[],"product_cat":[574],"product_tag":[3210,3211,3212,3213,793,2225,2305,2550,2852,3180,3205,3206,3207,3208,3209],"class_list":["post-7777","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-journal-articles","product_tag-pulse-height-spectrum","product_tag-quasi-monoenergetic","product_tag-response-to-neutrons","product_tag-silicon-carbides-sic","product_tag-energy-resolutions","product_tag-silicon-carbide","product_tag-solid-state-detectors","product_tag-neutrons","product_tag-monte-carlo-methods","product_tag-neutron-scattering","product_tag-nuclear-reactions","product_tag-silicon-detectors","product_tag-spalling","product_tag-detection-efficiency","product_tag-neutron-cross-sections","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/7777","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product"}],"about":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/types\/product"}],"replies":[{"embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/comments?post=7777"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media\/1294"}],"wp:attachment":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media?parent=7777"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=7777"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=7777"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}