{"id":8283,"date":"2024-09-15T19:38:12","date_gmt":"2024-09-15T16:38:12","guid":{"rendered":"https:\/\/quantum-electronics.ru\/en\/?p=8283"},"modified":"2024-09-16T13:58:56","modified_gmt":"2024-09-16T10:58:56","slug":"electric-discharge-krcl-laser-with-high-pump-power","status":"publish","type":"post","link":"https:\/\/quantum-electronics.ru\/en\/electric-discharge-krcl-laser-with-high-pump-power\/","title":{"rendered":"Electric-discharge KrCl laser with high pump power"},"content":{"rendered":"<p>S. A. Yampol\u2019skaya, A. G. Yastremskii, Yu. N. Panchenko, A. V. Puchikin, E. V. Gorlov<\/p>\n<ul>\n<li>Institute of High Current Electronics, Siberian Branch of the Russian Academy of Sciences, 634055, Tomsk, Russia<\/li>\n<li>National Research Tomsk State University, 634050, Tomsk, Russia<\/li>\n<li>Zuev Institute of Atmospheric Optics, Siberian Branch, Russian Academy of Sciences, 634055, Tomsk, Russia<\/li>\n<\/ul>\n<div class=\"around-button\"><b>Abstract:<\/b> The results of experimental and theoretical studies of the operation of the electric-discharge KrCl laser (<i>\u03bb<\/i> = 222 nm) at pump power densities of \u223c10 MW\/cm<sup>3<\/sup> are presented. The radiation energy of 55 mJ for the mixture with He as a buffer gas and 120 mJ for the mixture with Ne at pump pulse duration of \u223c30 ns was experimentally obtained. The numerical model of the KrCl laser using the He\/Ne\/Kr\/HCl gas mixture with a uniform pump discharge is described. It is numerically shown that the dependence of the optimal (from the point of view of obtaining the maximum radiation energy) pump power density on the partial pressures of the buffer gas and HCl is close to the linear one.<\/div>\n<div class=\"around-button\"><b>Keywords:<\/b> <i>electric-discharge KrCl laser, numerical simulation of laser mode<\/i><\/div>\n<div><\/div>\n<div><b>Received:<\/b> 28.02.2023<br \/>\n<b>Revised:<\/b> 18.04.2023<\/div>\n","protected":false},"excerpt":{"rendered":"<p>S. A. Yampol\u2019skaya, A. G. Yastremskii, Yu. N. Panchenko, A. V. Puchikin, E. V. Gorlov Institute of High Current Electronics, Siberian Branch of the Russian Academy of Sciences, 634055, Tomsk, Russia National Research Tomsk State University, 634050, Tomsk, Russia Zuev Institute of Atmospheric Optics, Siberian Branch, Russian Academy of Sciences, 634055, Tomsk, Russia Abstract: The\u2026 <span class=\"read-more\"><a href=\"https:\/\/quantum-electronics.ru\/en\/electric-discharge-krcl-laser-with-high-pump-power\/\">Read More &raquo;<\/a><\/span><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-8283","post","type-post","status-publish","format-standard","hentry","category-stats"],"_links":{"self":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/posts\/8283","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/comments?post=8283"}],"version-history":[{"count":0,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/posts\/8283\/revisions"}],"wp:attachment":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/media?parent=8283"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/categories?post=8283"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/tags?post=8283"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}