{"id":4804,"date":"2023-10-13T15:27:06","date_gmt":"2023-10-13T13:27:06","guid":{"rendered":"https:\/\/www.institut-foton.eu\/?p=4804"},"modified":"2025-07-16T16:40:28","modified_gmt":"2025-07-16T14:40:28","slug":"effets-transverses-dans-les-lasers","status":"publish","type":"post","link":"https:\/\/www.institut-foton.eu\/en\/effets-transverses-dans-les-lasers\/","title":{"rendered":"Spatial transverse effects in lasers"},"content":{"rendered":"<\/p>\n\n\n\n\n\n<figure class=\"wp-block-post-featured-image\"><img loading=\"lazy\" decoding=\"async\" width=\"858\" height=\"859\" src=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/Image_Effets-transverses.png\" class=\"attachment-post-thumbnail size-post-thumbnail wp-post-image\" alt=\"\" style=\"object-fit:cover;\" srcset=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/Image_Effets-transverses.png 858w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/Image_Effets-transverses-300x300.png 300w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/Image_Effets-transverses-150x150.png 150w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/Image_Effets-transverses-768x769.png 768w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/Image_Effets-transverses-270x270.png 270w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/Image_Effets-transverses-230x230.png 230w\" sizes=\"auto, (max-width: 858px) 100vw, 858px\" \/><\/figure>\n\n\n<h2 class=\"wp-block-heading\">Presentation<\/h2>\n\n\n\n<p>The excitation of higher order transverse modes in laser cavities has been studied for a long time, because certain modes have very interesting characteristics. As an example, \u201cvortex\u201d type Laguerre-Gauss modes transport orbital angular momentum; Bessel and Airy beams somehow \u201cresist\u201d diffraction, and are of interest for imaging and optical manipulation of micro- and nanoparticles. We study how structured transverse profiles emerge from the coupling between the spatial distribution of laser gain and the edge conditions imposed by the resonator.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">Partial degeneracy and excitation of higher order modes<\/h3>\n\n\n\n<p>It has been suggested that it is possible to excite higher order Laguerre-Gauss or Ince-Gauss modes in an optically pumped plano-concave cavity, by optimally positioning the focus point of the pump laser in the plane transverse and properly adjusting its size. We have shown theoretically, on the basis of an overlap integral between the gain and the modal profile, that the excitation of higher order modes with circular or elliptical nodal lines is only possible in the presence of a partial degeneration of the cavity. In this case, we generally obtain a superposition of modes of different order, giving rise to a transverse profile which is not invariant during propagation.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"542\" src=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/effets_transverses_lasers-image2-1024x542.png\" alt=\"\" class=\"wp-image-4806\" srcset=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/effets_transverses_lasers-image2-1024x542.png 1024w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/effets_transverses_lasers-image2-300x159.png 300w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/effets_transverses_lasers-image2-768x407.png 768w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/effets_transverses_lasers-image2.png 1386w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\">Fig.1 a) Quasi-Laguerre-Gauss mode. (b) Quasi-Ince-Gauss mode. NF: near field. FF: far field. The experiments are compared to Fox-Li (FL) type simulations.<\/figcaption><\/figure>\n\n\n\n<h3 class=\"wp-block-heading\">Waves and rays&nbsp;optics: geometric modes<\/h3>\n\n\n\n<p>Partial degeneracy effects also manifest themselves in a spectacular manner in so-called \u201cgeometric\u201d modes, whose properties can be understood in terms of ray optics.<\/p>\n\n\n\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"667\" height=\"661\" src=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/effets_transverses_lasers-image3.png\" alt=\"\" class=\"wp-image-4807\" srcset=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/effets_transverses_lasers-image3.png 667w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/effets_transverses_lasers-image3-300x297.png 300w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/effets_transverses_lasers-image3-150x150.png 150w\" sizes=\"auto, (max-width: 667px) 100vw, 667px\" \/><figcaption class=\"wp-element-caption\">Fig.2 Experimental observation and Fox-Li simulation of a geometric mode W, obtained by off-axis pumping of a degenerate plano-concave cavity of order 4 (L = Rc\/2).<\/figcaption><\/figure>\n\n\n\n<h2 class=\"wp-block-heading\">Financial support<\/h2>\n\n\n\n<ul class=\"puce1 wp-block-list\">\n<li><a href=\"https:\/\/www.univ-rennes.fr\/\" data-type=\"link\" data-id=\"https:\/\/www.univ-rennes.fr\/\">Universit\u00e9 de <\/a><a href=\"https:\/\/www.univ-rennes.fr\/\" data-type=\"link\" data-id=\"https:\/\/www.univ-rennes.fr\/\" target=\"_blank\" rel=\"noreferrer noopener\">Rennes<\/a><\/li>\n\n\n\n<li><a href=\"https:\/\/www.enseignementsup-recherche.gouv.fr\/fr\" data-type=\"link\" data-id=\"https:\/\/www.enseignementsup-recherche.gouv.fr\/fr\" target=\"_blank\" rel=\"noreferrer noopener\">Minist\u00e8re de l\u2019Enseignement Sup\u00e9rieur et de la Recherche<\/a><\/li>\n<\/ul>\n\n\n\n<h2 class=\"wp-block-heading\">Research staff involved<\/h2>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-28f84493 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<div class=\"wp-block-query is-layout-flow wp-block-query-is-layout-flow\">\n<div class=\"wp-block-group is-layout-constrained wp-block-group-is-layout-constrained\"><\/div>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<div class=\"wp-block-query is-layout-flow wp-block-query-is-layout-flow\">\n<div class=\"wp-block-group is-layout-constrained wp-block-group-is-layout-constrained\"><\/div>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<div class=\"wp-block-query is-layout-flow wp-block-query-is-layout-flow\">\n<div class=\"wp-block-group is-layout-constrained wp-block-group-is-layout-constrained\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n\n\n\n<h2 class=\"wp-block-heading\">To learn more&#8230;<\/h2>\n\n\n\n<ul class=\"puce1 ecartplus wp-block-list\">\n<li>Nicolas Barr\u00e9, Marco Romanelli, Marc Brunel. Role of cavity degeneracy for high-order mode excitation in end-pumped solid-state lasers. <em>Optics Letters<\/em>, 2014, 39 (4), pp.1022-1025. <a rel=\"noreferrer noopener\" href=\"https:\/\/dx.doi.org\/10.1364\/OL.39.001022\" target=\"_blank\">\u27e810.1364\/OL.39.001022\u27e9<\/a>. <a rel=\"noreferrer noopener\" href=\"https:\/\/hal.science\/hal-00947789\" target=\"_blank\">\u27e8hal-00947789\u27e9<\/a><\/li>\n\n\n\n<li>Nicolas Barr\u00e9, Marco Romanelli, M Lebental, Marc Brunel. Waves and rays in plano-concave laser cavities, part I. Geometric modes in the paraxial approximation. <em>European Journal of Physics<\/em>, 2017, 38 (3), pp.034010. <a rel=\"noreferrer noopener\" href=\"https:\/\/dx.doi.org\/10.1088\/1361-6404\/aa6461\" target=\"_blank\">\u27e810.1088\/1361-6404\/aa6461\u27e9<\/a>. <a rel=\"noreferrer noopener\" href=\"https:\/\/hal.science\/hal-01529983\" target=\"_blank\">\u27e8hal-01529983\u27e9<\/a><\/li>\n\n\n\n<li>A. Pascal, S. Bittner, B. Dietz, A. Trabattoni, C. Ulysse, et al.. Waves and rays in plano-concave laser cavities: II. A semiclassical approach. <em>European Journal of Physics<\/em>, 2017, 38 (3), pp.034011. <a rel=\"noreferrer noopener\" href=\"https:\/\/dx.doi.org\/10.1088\/1361-6404\/aa609d\" target=\"_blank\">\u27e810.1088\/1361-6404\/aa609d\u27e9<\/a>. <a rel=\"noreferrer noopener\" href=\"https:\/\/univ-rennes.hal.science\/hal-01517504\" target=\"_blank\">\u27e8hal-01517504\u27e9<\/a><\/li>\n<\/ul>\n\n\n<p>","protected":false},"excerpt":{"rendered":"<p>Presentation The excitation of higher order transverse modes in laser cavities has been studied for a long time, because certain modes have very interesting characteristics. As an example, \u201cvortex\u201d type Laguerre-Gauss modes transport orbital angular momentum; Bessel and Airy beams<\/p>\n","protected":false},"author":3,"featured_media":8478,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"inline_featured_image":false,"footnotes":""},"categories":[61],"tags":[30,108,46,93],"class_list":["post-4804","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-activites","tag-axe1","tag-departement-dop","tag-dynamique-lasers","tag-imagerie"],"translation":{"provider":"WPGlobus","version":"3.0.2","language":"en","enabled_languages":["fr","en"],"languages":{"fr":{"title":true,"content":true,"excerpt":false},"en":{"title":true,"content":true,"excerpt":false}}},"_links":{"self":[{"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts\/4804","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/comments?post=4804"}],"version-history":[{"count":12,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts\/4804\/revisions"}],"predecessor-version":[{"id":11213,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts\/4804\/revisions\/11213"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/media\/8478"}],"wp:attachment":[{"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/media?parent=4804"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/categories?post=4804"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/tags?post=4804"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}