{"id":6651,"date":"2021-02-01T17:58:33","date_gmt":"2021-02-01T17:58:33","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=6651"},"modified":"2022-06-21T09:57:14","modified_gmt":"2022-06-21T09:57:14","slug":"electron-impact-state-to-state-cross-sections-and-rate-coefficients-for-xv-av-excitation-of-lih-molecule","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/electron-impact-state-to-state-cross-sections-and-rate-coefficients-for-xv-av-excitation-of-lih-molecule\/","title":{"rendered":"Electron-impact state-to-state cross sections and rate coefficients for X(v)->A(v&#8217;) excitation of LiH molecule"},"content":{"rendered":"<p>Electron-impact cross sections for the v->V&#8217;transitions between the vibrational levels of X ? and A ? electronic states of the LiH molecule, are calculated from threshold to 1000 eV by using the threshold-modified Massey-Mott approximation. The rate coefficients for the same transitions are also calculated in the range 0.1-1000 eV. Scaling relationships for both the v &#8211; v? cross section and v &#8211; v? rate coefficients are derived, allowing us to represent the calculated quantities in a compact analytic form.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Celiberto R.; Janev R.K.; Laricchiuta A.<\/p>\n","protected":false},"featured_media":1294,"comment_status":"closed","ping_status":"open","template":"","meta":[],"product_cat":[574],"product_tag":[1044,1045],"class_list":["post-6651","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-journal-articles","product_tag-electron-molecule-cross-sections","product_tag-excited-states","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/6651","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=6651"}],"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=6651"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=6651"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=6651"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}