{"id":7300,"date":"2019-07-29T13:41:49","date_gmt":"2019-07-29T13:41:49","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=7300"},"modified":"2023-02-14T10:01:42","modified_gmt":"2023-02-14T10:01:42","slug":"theory-based-investigation-of-outer-mode-to-elm-transition-in-jet-c-plasmas","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/theory-based-investigation-of-outer-mode-to-elm-transition-in-jet-c-plasmas\/","title":{"rendered":"Theory based investigation of Outer Mode to ELM transition in JET-C plasmas"},"content":{"rendered":"<p>Tokamak high-confinement regimes are normally affected by the presence of often violent edge localised modes (ELMs). ELMs deposit unacceptable peak heat loads causing a severe deterioration of the plasma facing components. Although several ELM control\/suppression techniques have been developed, they may not be applicable to future reactors such as ITER and DEMO. Thus a vivid interest has arisen on the development of naturally ELM-free regimes. One of the most promising of such regimes is the so called quiescent high-confinement (QH) mode. In QH plasmas, ELM activity is replaced by dominantly low-n steady mild rotating MHD edge harmonic oscillations (EHOs) localised in the pedestal region. EHOs have been observed in DIII-D, ASDEX-U, JET and JT60 [1]. In JET such a MHD activity is referred to as Outer Modes (OMs) [2].<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Brunetti D.; Graves J.P.; Lazzaro E.; Mariani A.; Nowak S.; Cooper W.A.; Wahlberg C.; Solano E.R.; Saarelma S.; JET Contributors<\/p>\n","protected":false},"featured_media":1294,"comment_status":"closed","ping_status":"open","template":"","meta":[],"product_cat":[704],"product_tag":[2299,2300],"class_list":["post-7300","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-conference-proceedings","product_tag-elm-transition","product_tag-jet-c-plasmas","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/7300","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=7300"}],"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=7300"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=7300"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=7300"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}