{"id":5332,"date":"2021-11-22T12:52:31","date_gmt":"2021-11-22T11:52:31","guid":{"rendered":"https:\/\/laser.usal.es\/alf\/?p=5332"},"modified":"2022-01-17T13:39:02","modified_gmt":"2022-01-17T12:39:02","slug":"the-lord-of-the-rings-the-graphene-match","status":"publish","type":"post","link":"https:\/\/laser.usal.es\/attostructura\/en\/2021\/11\/22\/the-lord-of-the-rings-the-graphene-match\/","title":{"rendered":"The Lord of the Rings: the Graphene Match"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-post\" data-elementor-id=\"5332\" class=\"elementor elementor-5332\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-3cdefe61 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"3cdefe61\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-7f5285e\" data-id=\"7f5285e\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-43341958 elementor-widget elementor-widget-text-editor\" data-id=\"43341958\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<div class=\"\" dir=\"auto\" style=\"text-align: justify;\"><div><span lang=\"EN-US\">As in the books of JRR Tolkien, the Research Group of Laser Applications and Photonics (ALF-USAL) continues their adventure in the search of the Ring<\/span><span lang=\"EN-US\">.<\/span><\/div><div>\u00a0<\/div><div><div><span lang=\"EN-US\">After finding the Phase-Matched Ring in Argon based High-Harmonic Generation [1], now they\u2019ve gone a step beyond to find the Phase-Matched Ring in graphene. It turns out that when a graphene layer is illuminated by an intense laser beam, ultrafast electronic dynamics result in the emission of higher frequency radiation. <\/span><\/div><div>\u00a0<\/div><\/div><div><span lang=\"EN-US\">This emission can be understood as a result of an excitation of electrons from the valence to the conduction band, a subsequent acceleration in such conduction band, and a final recombination with the holes that were left in the valence band. Such process, known as high-order harmonic generation, is very sensitive to the intensity of the incoming laser field, and thus to the spatial profile of the beam. <\/span><\/div><div>\u00a0<\/div><div><span lang=\"EN-US\">As a consequence, the radiation emitted from different parts of the graphene layer can interfere, both destructively or constructively. It turns out that an adequate matching between the emissions from different parts of the graphene layer is required to obtain bright high-frequency radiation.<\/span><\/div><div>\u00a0<\/div><div><div><span lang=\"EN-US\">In their latest work, the ALF-USAL group has demonstrated that when a graphene layer is illuminated by an intense Gaussian beam, the high-order harmonic emission is dominated by an annular region: the Phase-Matched Ring. This finding gives light into the macroscopic physics of high harmonic generation in graphene, offering a tool to engineer the process, and to increase its efficiency.<\/span><\/div><div>\u00a0<\/div><\/div><div><span lang=\"EN-US\">After finding the Phase-Matched Ring in Argon and in Graphene, the researchers of ALF-USAL group continue their adventures to rule intense light-matter interactions.<\/span><\/div><div>\u00a0<\/div><div><p><em><span lang=\"EN-US\">More information in:\u00a0<\/span><\/em><\/p><\/div><div><p><a href=\"https:\/\/www.osapublishing.org\/oe\/fulltext.cfm?uri=oe-29-2-2488&amp;id=446590\"><span lang=\"EN-US\">\u201cTransverse phase matching of high-order harmonic generation in single-layer graphene\u201d<\/span><\/a><span lang=\"EN-US\">, Roberto Boyero-Garc\u00eda, \u00d3scar Zurr\u00f3n-Cifuentes, Luis Plaja, and Carlos Hern\u00e1ndez-Garc\u00eda,\u00a0\u00a0<b><i>Optics Express 29,<\/i><\/b><i>\u00a02488-2500\u00a0(2021).<\/i><\/span><\/p><\/div><div><p><i><span lang=\"EN-US\">References:<\/span><\/i><\/p><\/div><div><p><i><span lang=\"EN-US\">[1] <\/span><\/i><a href=\"https:\/\/www.osapublishing.org\/oe\/abstract.cfm?uri=oe-23-16-21497\"><i><span lang=\"EN-US\">\u201cCarrier-envelope-phase insensitivity in high-order harmonic generation driven by few-cycle laser pulses\u201d<\/span><\/i><\/a><i><span lang=\"EN-US\">,\u00a0C. Hern\u00e1ndez-Garc\u00eda,\u00a0W. Holgado, L. Plaja, B. Alonso, F. Silva,\u00a0M. Miranda, H. Crespo, and I. J. Sola,\u00a0<b>Optics Express<\/b>\u00a0\u00a0<b>23<\/b>,\u00a021497\u00a0(2015)<\/span><\/i><\/p><\/div><div><p>Download in\u00a0Gredos@Universidad de Salamanca: <a href=\"http:\/\/hdl.handle.net\/10366\/146004\">http:\/\/hdl.handle.net\/10366\/146004<\/a><\/p><\/div><\/div><div class=\"\">\u00a0<\/div>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-3a73625 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"3a73625\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-1ab1432\" data-id=\"1ab1432\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-4b7fe3c elementor-widget elementor-widget-image\" data-id=\"4b7fe3c\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img fetchpriority=\"high\" decoding=\"async\" width=\"300\" height=\"220\" src=\"https:\/\/laser.usal.es\/attostructura\/wp-content\/uploads\/2022\/01\/Logos-300x220.png\" class=\"attachment-medium size-medium wp-image-6339\" alt=\"\" srcset=\"https:\/\/laser.usal.es\/attostructura\/wp-content\/uploads\/2022\/01\/Logos-300x220.png 300w, https:\/\/laser.usal.es\/attostructura\/wp-content\/uploads\/2022\/01\/Logos-768x562.png 768w, https:\/\/laser.usal.es\/attostructura\/wp-content\/uploads\/2022\/01\/Logos.png 850w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>As in the books of JRR Tolkien, the Research Group of Laser Applications and Photonics (ALF-USAL) continues their adventure in the search of the Ring.\u00a0After finding the Phase-Matched Ring in Argon based High-Harmonic Generation [1], now they\u2019ve gone a step beyond to find the Phase-Matched Ring in graphene. It turns out that when a graphene<\/p>\n","protected":false},"author":2,"featured_media":5337,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"categories":[385,402],"tags":[],"class_list":["post-5332","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-attostructura-en","category-review"],"_links":{"self":[{"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/posts\/5332","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/comments?post=5332"}],"version-history":[{"count":7,"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/posts\/5332\/revisions"}],"predecessor-version":[{"id":6351,"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/posts\/5332\/revisions\/6351"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/media\/5337"}],"wp:attachment":[{"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/media?parent=5332"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/categories?post=5332"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/laser.usal.es\/attostructura\/wp-json\/wp\/v2\/tags?post=5332"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}