{"id":2492,"date":"2021-05-26T00:00:44","date_gmt":"2021-05-26T00:00:44","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=2492"},"modified":"2022-05-29T16:30:28","modified_gmt":"2022-05-29T16:30:28","slug":"first-spatially-resolved-measurements-of-the-d-3he-alpha-particle-source-with-the-upgraded-jet-gamma-ray-camera","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/first-spatially-resolved-measurements-of-the-d-3he-alpha-particle-source-with-the-upgraded-jet-gamma-ray-camera\/","title":{"rendered":"First spatially resolved measurements of the D-3He alpha-particle source with the upgraded JET gamma-ray camera"},"content":{"rendered":"<p>The Joint European Torus (JET) gamma-ray camera has been recently upgraded with the installation of new gamma-ray detectors, based on LaBr3(Ce) scintillation crystals, which add spectroscopic capability to the existing system allowing measurements with good energy resolution (5% at 0.622 MeV), a dynamic range from hundreds of keV up to about 30 MeV, and high counting rate capabilities of MCps. First gamma-ray measurements during the C38 campaign of the JET have been successfully carried out, in particular, in D-3He plasmas from three-ion ion cyclotron resonance heating experiments, where the detection of 16.4 MeV y-rays from D + 3He -> y + 5Li reactions with the gamma-ray camera upgrade allowed determining the spatial profile of alpha particles born in D + 3He fusion reactions.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Panontin E.; Rigamonti D.; Nocente M.; Dal Molin A.; Broslawski A.; Craciunescu T.; Croci G.; Cruz N.; Figueiredo J.; Giacomelli L.; Gorini G.; Gosk M.; Kaveney G.; Kazakov Y.O.; Kiptily V.; Korolczuk S.; Marcer G.; Murari A.; Perelli Cippo E.; Salewski M.; Urban A.; Zychor I.; Tardocchi M.<\/p>\n","protected":false},"featured_media":2693,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"product_cat":[574,524],"product_tag":[789,790,791,792,793,794,795,796,797,798,799,800],"class_list":["post-2492","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-journal-articles","product_cat-thermonuclear-fusion","product_tag-gamma-rays","product_tag-alpha-particles","product_tag-cameras","product_tag-cyclotron-resonance","product_tag-energy-resolutions","product_tag-gamma-ray-detector","product_tag-gamma-ray-measurements","product_tag-gamma-ray-cameras","product_tag-ion-cyclotron-resonance-heating","product_tag-joint-european-torus","product_tag-scintillation-crystals","product_tag-spatially-resolved","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/2492","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=2492"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media\/2693"}],"wp:attachment":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media?parent=2492"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=2492"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=2492"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}