{"id":7175,"date":"2021-01-26T13:46:12","date_gmt":"2021-01-26T13:46:12","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=7175"},"modified":"2022-06-21T10:35:45","modified_gmt":"2022-06-21T10:35:45","slug":"reactive-collisions-between-electrons-and-bet","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/reactive-collisions-between-electrons-and-bet\/","title":{"rendered":"Reactive collisions between electrons and BeT+"},"content":{"rendered":"<p>In order to model and diagnose the low-temperature edge plasmas, a complete database for electron-impact collision processes is required for molecular species containing beryllium and hydrogen. Dominant elementary processes in cold ionized gases are dissociative recombination, elastic collisions, vibrational excitation, vibrational de-excitation and dissociative excitation. In this study, using the stepwise version of the Multichannel Quantum Defect Theory, cross sections and rate coefficients have been obtained for reactions induced on BeT+. A set of vibrational resolved rate coefficients for BeT+ cations&#8217; reactive collisions with electrons below to the ion dissociation threshold is provided. The incident electron energy range is 10-3 &#8211; 2.7 eV and the electron temperature range is 100 &#8211; 5000 K.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Iacob, F.; Pop, N.; Mezei, J. Zs.; Niyonzima, S.; Laporta, V.; Chakrabarti, K.; Schneider, I. F.<\/p>\n","protected":false},"featured_media":1294,"comment_status":"closed","ping_status":"open","template":"","meta":[],"product_cat":[704],"product_tag":[2062,2063],"class_list":["post-7175","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-conference-proceedings","product_tag-low-temperature-edge-plasmas","product_tag-international-thermonuclear-experimental-reactor-iter","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/7175","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=7175"}],"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=7175"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=7175"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=7175"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}