{"id":7844,"date":"2024-09-13T11:19:07","date_gmt":"2024-09-13T08:19:07","guid":{"rendered":"https:\/\/quantum-electronics.ru\/en\/?p=7844"},"modified":"2024-09-13T13:13:46","modified_gmt":"2024-09-13T10:13:46","slug":"synchronously-pumped-anti-stokes-raman-parametric-laser-on-a-camoo4-crystal","status":"publish","type":"post","link":"https:\/\/quantum-electronics.ru\/en\/synchronously-pumped-anti-stokes-raman-parametric-laser-on-a-camoo4-crystal\/","title":{"rendered":"Synchronously pumped anti-Stokes Raman-parametric laser on a CaMoO4 crystal"},"content":{"rendered":"<p>S. N. Smetanin, D. P. Tereshchenko, A. G. Papashvili, E. V. Shashkov, M. D. Lapina, V. E. Shukshin, K. A. Subbotin, D. A. Lis, A. I. Titov<\/p>\n<p>Prokhorov General Physics Institute of the Russian Academy of Sciences, Moscow<\/p>\n<div class=\"around-button\"><b>Abstract:<\/b> We study generation of a crystalline anti-Stokes Raman-parametric laser with collinear phase-matching under intracavity synchronous pumping by a 1064-nm, passively <i>Q<\/i>-switched, longitudinally mode-locked Nd<sup>3+<\/sup>:YAG laser. As an active medium, use is made of a CaMoO<sub>4<\/sub> crystal, which has optimal birefringence for the angular phase-mismatching insensitive Stokes-anti-Stokes Raman-parametric four-wave interaction at a matching angle of 71\u00b0 and an angular matching width of 4\u00b0. The conditions are determined for generating a single ultrashort anti-Stokes pulse at a wavelength of 973 nm with a pulse duration of 9 ps and an energy of up to 9 \u03bcJ.<\/div>\n<div><\/div>\n<div class=\"around-button\"><b>Keywords:<\/b> <i>stimulated Raman scattering, parametric Raman laser, anti-Stokes radiation, phase matching.<\/i><\/div>\n<div><\/div>\n<div><b>Received:<\/b> 10.08.2022<\/div>\n","protected":false},"excerpt":{"rendered":"<p>S. N. Smetanin, D. P. Tereshchenko, A. G. Papashvili, E. V. Shashkov, M. D. Lapina, V. E. Shukshin, K. A. Subbotin, D. A. Lis, A. I. Titov Prokhorov General Physics Institute of the Russian Academy of Sciences, Moscow Abstract: We study generation of a crystalline anti-Stokes Raman-parametric laser with collinear phase-matching under intracavity synchronous pumping\u2026 <span class=\"read-more\"><a href=\"https:\/\/quantum-electronics.ru\/en\/synchronously-pumped-anti-stokes-raman-parametric-laser-on-a-camoo4-crystal\/\">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":[3038,1729,1735,1732,1734,1730,1733,1731,1727],"class_list":["post-7844","post","type-post","status-publish","format-standard","hentry","category-stats","tag-d-p-tereshchenko","tag-a-g-papashvili","tag-a-i-titov","tag-v-e-shukshin","tag-d-a-lis","tag-e-v-shashkov","tag-k-a-subbotin","tag-m-d-lapina","tag-s-n-smetanin"],"_links":{"self":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/posts\/7844","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=7844"}],"version-history":[{"count":0,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/posts\/7844\/revisions"}],"wp:attachment":[{"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/media?parent=7844"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/categories?post=7844"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/quantum-electronics.ru\/en\/wp-json\/wp\/v2\/tags?post=7844"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}