{"id":7917,"date":"2022-04-26T11:44:18","date_gmt":"2022-04-26T11:44:18","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=7917"},"modified":"2023-02-08T17:02:05","modified_gmt":"2023-02-08T17:02:05","slug":"gamma-ray-measurements-in-d3he-fusion-plasma-experiments-on-jet","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/gamma-ray-measurements-in-d3he-fusion-plasma-experiments-on-jet\/","title":{"rendered":"Gamma-ray measurements in D3He fusion plasma experiments on JET"},"content":{"rendered":"<p>Using capabilities of the gamma-ray spectrometry, fusion born alpha-particles were studied in recent D-3He plasma experiments on JET. A substantial population of the alpha-particles was generated in the 3He-rich plasma due to the 3He(D, p)4He reaction. Fast deuterium ions of the neutral beam injection (NBI) heating were accelerated to MeV energies with three-ion scenario D-(DNBI)-3He using radio frequency waves in the ion cyclotron range of frequencies (ICRF). A high reaction rate allowed to measure the alpha-particle production rate and their spatial distribution in the plasma by detecting 16.7-MeV gamma-rays from the 3He(D, y)5 Li reaction, which is a weak branch of 3He(D, p)4He reaction. A branching ratio of gamma-ray transitions to the ground and the first excited states of 5Li was obtained. Due to the beryllium is a main impurity of JET plasmas, intensive gamma-rays from the Be-9(D, ny) 10B, Be-9(D, py) 10Be and Be-9(a, ny) C-12 reactions were observed. Exploitation of the reaction cross-sections and the Doppler shape analysis (DSA) of gamma-lines in the recorded spectra provided the possibility to reconstruct distribution functions of the confined D-ions and the fusion-born alpha-particles.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Iliasova M.; Shevelev A.; Khilkevich E.; Kazakov Y; Kiptily V.; Nocente M.; Giacomelli L.; Craciunescu T.; Stancar Z.; Dal Molin A.; Rigamonti D.; Tardocchi M.; Doinikov D.; Gorini G.; Naidenov V.; Polunovsky I.; Gin D.<\/p>\n","protected":false},"featured_media":1294,"comment_status":"closed","ping_status":"open","template":"","meta":[],"product_cat":[574],"product_tag":[790,1500,2374,2647,3429],"class_list":["post-7917","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-journal-articles","product_tag-alpha-particles","product_tag-tokamak-plasma","product_tag-gamma-ray-spectrometry","product_tag-fusion-reaction","product_tag-fusion-rate","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/7917","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=7917"}],"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=7917"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=7917"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=7917"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}