{"id":1632,"date":"2023-02-08T09:10:59","date_gmt":"2023-02-08T09:10:59","guid":{"rendered":"https:\/\/www.nanosciences-spm-uhv.com\/?p=1632"},"modified":"2025-11-05T16:58:24","modified_gmt":"2025-11-05T16:58:24","slug":"pub2","status":"publish","type":"post","link":"https:\/\/www.nanosciences-spm-uhv.com\/en\/pub2\/","title":{"rendered":"Mapping Lamb, Stark, and Purcell Effects at a Chromophore-Picocavity Junction with Hyper-Resolved Fluorescence Microscopy"},"content":{"rendered":"<p class=\"wp-block-paragraph\">The interactions of the excited states of a single chromophore with static and dynamic electric fields spatially varying at the atomic scale are investigated in a joint experimental and theoretical effort. In this configuration, the spatial extension of the fields confined at the apex of a scanning tunneling microscope tip is smaller than that of the molecular exciton, a property used to generate fluorescence maps of the chromophore with intramolecular resolution. Theoretical simulations of the electrostatic and electrodynamic interactions occurring at the picocavity junction formed by the chromophore, the tip, and the substrate reveal the key role played by subtle variations of Purcell, Lamb, and Stark effects. They also demonstrate that hyper-resolved fluorescence maps of the line shift and linewidth of the excitonic emission can be understood as images of the static charge redistribution upon electronic excitation of the molecule and as the distribution of the dynamical charge oscillation associated with the molecular exciton, respectively.<\/p>\n\n\n\n<div style=\"height:37px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<div class=\"wp-block-uagb-buttons uagb-buttons__outer-wrap uagb-btn__default-btn uagb-btn-tablet__default-btn uagb-btn-mobile__default-btn uagb-block-4f821bde\"><div class=\"uagb-buttons__wrap uagb-buttons-layout-wrap\">\n<div class=\"wp-block-uagb-buttons-child uagb-buttons__outer-wrap uagb-block-7018d71a wp-block-button is-style-outline\"><div class=\"uagb-button__wrapper\"><a class=\"uagb-buttons-repeater wp-block-button__link has-text-color\" href=\"https:\/\/journals.aps.org\/prx\/abstract\/10.1103\/PhysRevX.12.011012\" onclick=\"return true;\" rel=\"follow noopener\" target=\"_blank\"><div class=\"uagb-button__link\">Full text<\/div><span class=\"uagb-button__icon uagb-button__icon-position-after\"><svg xmlns=\"https:\/\/www.w3.org\/2000\/svg\" viewbox=\"0 0 448 512\"><path d=\"M438.6 278.6l-160 160C272.4 444.9 264.2 448 256 448s-16.38-3.125-22.62-9.375c-12.5-12.5-12.5-32.75 0-45.25L338.8 288H32C14.33 288 .0016 273.7 .0016 256S14.33 224 32 224h306.8l-105.4-105.4c-12.5-12.5-12.5-32.75 0-45.25s32.75-12.5 45.25 0l160 160C451.1 245.9 451.1 266.1 438.6 278.6z\"><\/path><\/svg><\/span><\/a><\/div><\/div>\n\n\n\n<div class=\"wp-block-uagb-buttons-child uagb-buttons__outer-wrap uagb-block-2458f534 wp-block-button is-style-outline\"><div class=\"uagb-button__wrapper\"><a class=\"uagb-buttons-repeater wp-block-button__link has-text-color\" href=\"https:\/\/www.nanosciences-spm-uhv.com\/en\/gdr\/publications\/\" onclick=\"return true;\" rel=\"follow noopener\" target=\"_self\"><div class=\"uagb-button__link\">Back to publications<\/div><span class=\"uagb-button__icon uagb-button__icon-position-after\"><svg xmlns=\"https:\/\/www.w3.org\/2000\/svg\" viewbox=\"0 0 448 512\"><path d=\"M438.6 278.6l-160 160C272.4 444.9 264.2 448 256 448s-16.38-3.125-22.62-9.375c-12.5-12.5-12.5-32.75 0-45.25L338.8 288H32C14.33 288 .0016 273.7 .0016 256S14.33 224 32 224h306.8l-105.4-105.4c-12.5-12.5-12.5-32.75 0-45.25s32.75-12.5 45.25 0l160 160C451.1 245.9 451.1 266.1 438.6 278.6z\"><\/path><\/svg><\/span><\/a><\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-buttons is-layout-flex wp-block-buttons-is-layout-flex\"><\/div>\n<p>DOI : <a href=\"https:\/\/doi.org\/10.1103\/PhysRevX.12.011012\">10.1103\/PhysRevX.12.011012<\/a><\/p><p>Authors : Anna Ros\u0142awska, Tom\u00e1\u0161 Neuman, Benjamin Doppagne, Andrei G. Borisov, Michelangelo Romeo, Fabrice Scheurer, Javier Aizpurua, and Guillaume Schull<\/p>","protected":false},"excerpt":{"rendered":"<p>The interactions of the excited states of a single chromophore with static and dynamic electric fields spatially varying at the atomic scale are investigated in a joint experimental and theoretical effort. In this configuration, the spatial extension of the fields confined at the apex of a scanning tunneling microscope tip is smaller than that of<\/p><\/div>\n<div class=\"blog-btn\"><a href=\"https:\/\/www.nanosciences-spm-uhv.com\/en\/pub2\/\" class=\"home-blog-btn\">Read More<\/a><\/p>","protected":false},"author":1,"featured_media":1634,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_uag_custom_page_level_css":"","footnotes":""},"categories":[20,23],"tags":[],"class_list":["post-1632","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-axe2","category-axe5"],"uagb_featured_image_src":{"full":["https:\/\/www.nanosciences-spm-uhv.com\/wp-content\/uploads\/2023\/02\/Image1.jpg",320,320,false],"thumbnail":["https:\/\/www.nanosciences-spm-uhv.com\/wp-content\/uploads\/2023\/02\/Image1-150x150.jpg",150,150,true],"medium":["https:\/\/www.nanosciences-spm-uhv.com\/wp-content\/uploads\/2023\/02\/Image1-300x300.jpg",300,300,true],"medium_large":["https:\/\/www.nanosciences-spm-uhv.com\/wp-content\/uploads\/2023\/02\/Image1.jpg",320,320,false],"large":["https:\/\/www.nanosciences-spm-uhv.com\/wp-content\/uploads\/2023\/02\/Image1.jpg",320,320,false],"1536x1536":["https:\/\/www.nanosciences-spm-uhv.com\/wp-content\/uploads\/2023\/02\/Image1.jpg",320,320,false],"2048x2048":["https:\/\/www.nanosciences-spm-uhv.com\/wp-content\/uploads\/2023\/02\/Image1.jpg",320,320,false],"trp-custom-language-flag":["https:\/\/www.nanosciences-spm-uhv.com\/wp-content\/uploads\/2023\/02\/Image1-12x12.jpg",12,12,true],"sow-carousel-default":["https:\/\/www.nanosciences-spm-uhv.com\/wp-content\/uploads\/2023\/02\/Image1-272x182.jpg",272,182,true]},"uagb_author_info":{"display_name":false,"author_link":"https:\/\/www.nanosciences-spm-uhv.com\/en\/author\/zpqq18wlui98\/"},"uagb_comment_info":0,"uagb_excerpt":"The interactions of the excited states of a single chromophore with static and dynamic electric fields spatially varying at the atomic scale are investigated in a joint experimental and theoretical effort. In this configuration, the spatial extension of the fields confined at the apex of a scanning tunneling microscope tip is smaller than that ofRead&hellip;","_links":{"self":[{"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/posts\/1632","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/comments?post=1632"}],"version-history":[{"count":4,"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/posts\/1632\/revisions"}],"predecessor-version":[{"id":1803,"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/posts\/1632\/revisions\/1803"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/media\/1634"}],"wp:attachment":[{"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/media?parent=1632"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/categories?post=1632"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.nanosciences-spm-uhv.com\/en\/wp-json\/wp\/v2\/tags?post=1632"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}