{"id":9,"date":"2021-08-06T14:03:11","date_gmt":"2021-08-06T18:03:11","guid":{"rendered":"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/?page_id=9"},"modified":"2023-10-05T13:17:09","modified_gmt":"2023-10-05T17:17:09","slug":"page-built-using-the-new-editor","status":"publish","type":"page","link":"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/","title":{"rendered":"Welcome"},"content":{"rendered":"\n<figure class=\"wp-block-image size-large\"><img decoding=\"async\" width=\"1024\" height=\"729\" data-src=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/IMG_1529-1024x729.jpg\" alt=\"Colorful abstract art\" class=\"wp-image-349 lazyload\" data-srcset=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/IMG_1529-1024x729.jpg 1024w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/IMG_1529-300x214.jpg 300w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/IMG_1529-768x547.jpg 768w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/IMG_1529-1536x1094.jpg 1536w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/IMG_1529-2048x1458.jpg 2048w\" data-sizes=\"(max-width: 1024px) 100vw, 1024px\" src=\"data:image\/svg+xml;base64,PHN2ZyB3aWR0aD0iMSIgaGVpZ2h0PSIxIiB4bWxucz0iaHR0cDovL3d3dy53My5vcmcvMjAwMC9zdmciPjwvc3ZnPg==\" style=\"--smush-placeholder-width: 1024px; --smush-placeholder-aspect-ratio: 1024\/729;\" \/><figcaption class=\"wp-element-caption\">Enrico Prometti, tecnica mista su supporto ligneo, dettaglio. Bergamo 1972.<\/figcaption><\/figure>\n\n\n\n<h2 class=\"wp-block-heading\">A New Science is Born (and won the Nobel Prize!)<\/h2>\n\n\n\n<p>At the turn of the XX century, transformative advances in laser technology have led to the generation of light pulses with duration as short as few tens of attoseconds (1 as = 10<sup>-18<\/sup> s), which is the characteristic time scale of electrons&#8217; motion in atoms and molecules. This breakthrough made it possible to observe the most elementary processes in matter, such as charge migration, the photoelectric effect, and Auger decay, in real time.<\/p>\n\n\n\n<p>On October 3<sup>rd<\/sup> 2023, the Royal Swedish Academy of Sciences awarded the <a href=\"https:\/\/www.nobelprize.org\/prizes\/physics\/2023\/summary\/\">Nobel Prize in Physics to Pierre Agostini, Ferenc Krausz, and Anne <\/a><a href=\"https:\/\/www.nobelprize.org\/prizes\/physics\/2023\/summary\/\" target=\"_blank\" rel=\"noreferrer noopener\">L&#8217;Huillier<\/a> &#8220;for experimental methods that generate attosecond pulses of light for the study of electron dynamics in matter&#8221;. This major recognition highlights both the important contributions of these founding members of the attosecond community and the lasting impact of attosecond science on the field of physics. <\/p>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-9d6595d7 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<p>By virtue of the time-energy uncertainty principle, attosecond light pulses contain a broad range of frequencies that reach from the extreme ultraviolet to the x-ray region of the electromagnetic spectrum. The photon energy, therefore, is large enough to eject one or more electrons from a target. Attosecond spectroscopies, furthermore, often employ intense infrared probe pulses that trigger highly non-linear processes in the electronic continuum.<\/p>\n\n\n\n<p>Attosecond spectroscopies involves the ionization continuum and many non-perturbative processes, in which electronic correlation and quantum coherence play a major role. For these reasons, traditional perturbative tools designed for non-linear infrared and visible spectroscopies, electronic many-body methods for bound states, strong-field methods in single-particle approximation, and incoherent population-dynamics methods for plasmas, are insufficient to interpret and guide attosecond experiments. <\/p>\n\n\n\n<p>The Theoretical Attosecond Science group at UCF develops new ab initio theories, analytical and semi-empirical models, and computational methodologies that can simulate the ultrafast electronic and nuclear motion triggered by ultrashort light pulses in atoms and molecules. Learn more about <a href=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/people\/\">who we are<\/a>, <a href=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/research\/\">our research<\/a>, <a href=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/outreach\/\">outreach<\/a> activities, and <a href=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/publications\/\">publications<\/a>.<\/p>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-large\"><img decoding=\"async\" width=\"953\" height=\"1024\" data-src=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/8d_FormationFano-2-953x1024.png\" alt=\"Formation of a Fano profile over time. The image shows the probability of detecting a photoelectron in the energy region of the 2s2p auto ionizing state of the helium atom, as a function of the electron energy and of the time elapsed from the initial Attosecond excitation pulse. The picture shows how, for the first few femtosecond, the distribution is gaussian, as if there were no resonance: that is the electron distribution due to the direct non-resonant emission to the continuum. However, the light pulse has populated also the metastable 2s2p state. Over time, this state decays, and its partially decayed component interfere with the direct-ionization background to give rise to an emerging asymmetric peak superposed to several hyperbolic interference fringes. In the limit of infinite time, when the autoionizing state has fully decayed, the photoelectron spectrum coincides with the characteristic asymmetric profile (a.k.a. Fano profile) observed in stationary regime, e.g., at synchrotron-radiation facilities. With Attosecond science, however, it is possible to take a snapshot of the portion of the system in the continuum at finite time, and observe the formation of the peak over time.\" class=\"wp-image-200 lazyload\" data-srcset=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/8d_FormationFano-2-953x1024.png 953w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/8d_FormationFano-2-279x300.png 279w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/8d_FormationFano-2-768x825.png 768w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/8d_FormationFano-2.png 1214w\" data-sizes=\"(max-width: 953px) 100vw, 953px\" src=\"data:image\/svg+xml;base64,PHN2ZyB3aWR0aD0iMSIgaGVpZ2h0PSIxIiB4bWxucz0iaHR0cDovL3d3dy53My5vcmcvMjAwMC9zdmciPjwvc3ZnPg==\" style=\"--smush-placeholder-width: 953px; --smush-placeholder-aspect-ratio: 953\/1024;\" \/><figcaption class=\"wp-element-caption\">Emergence of the asymmetric profile in the electronic continuum of the 2s2p resonance of the helium atom, as a function of the time elapsed from the initial excitation of the atom by an attosecond pulse.<\/figcaption><\/figure>\n<\/div>\n<\/div>\n\n\n\n<h2 class=\"wp-block-heading\">Contact<\/h2>\n\n\n\n<p><a href=\"mailto:luca.argenti@ucf.edu\">luca.argenti@ucf.edu<\/a><\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Federal and Institutional Support<\/h2>\n\n\n\n<p>Since its inception in 2016, the research of Luca Argenti&#8217;s Theoretical Attosecond Science group at UCF has been generously supported by three consecutive 3-year grants from the Theoretical Atomic, Molecular, and Optical Physics (<a href=\"https:\/\/new.nsf.gov\/funding\/opportunities\/atomic-molecular-optical-physics-theory-0#:~:text=The%20Theoretical%20Atomic%2C%20Molecular%2C%20and,atoms%20and%20small%20molecules%2C%20time%2D\">TAMOP<\/a>) Program of the National Science Foundation, and by a 5-year Early Career award from the Atomic, Molecular, and Optical Sciences (<a href=\"https:\/\/science.osti.gov\/bes\/csgb\/Research-Areas\/Atomic-Molecular-and-Optical-Science\">AMOS<\/a>) Program of the Department of Energy. The group gratefully acknowledges also UCF support through the PI&#8217;s starting grant, seed funds, the Reach For The Stars award, and four Preeminent Postdoctoral Scholar awards (P<sup>3<\/sup>), which have been instrumental in multiplying federal grant&#8217;s impact.<\/p>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-9d6595d7 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-large\"><a href=\"https:\/\/www.nsf.gov\"><img decoding=\"async\" width=\"1019\" height=\"1024\" data-src=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/National_Science_Foundation_logo_PNG1-1019x1024.png\" alt=\"National Science Foundation Logo\" class=\"wp-image-278 lazyload\" data-srcset=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/National_Science_Foundation_logo_PNG1-1019x1024.png 1019w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/National_Science_Foundation_logo_PNG1-298x300.png 298w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/National_Science_Foundation_logo_PNG1-150x150.png 150w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/National_Science_Foundation_logo_PNG1-768x772.png 768w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/National_Science_Foundation_logo_PNG1-1528x1536.png 1528w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/National_Science_Foundation_logo_PNG1.png 1722w\" data-sizes=\"(max-width: 1019px) 100vw, 1019px\" src=\"data:image\/svg+xml;base64,PHN2ZyB3aWR0aD0iMSIgaGVpZ2h0PSIxIiB4bWxucz0iaHR0cDovL3d3dy53My5vcmcvMjAwMC9zdmciPjwvc3ZnPg==\" style=\"--smush-placeholder-width: 1019px; --smush-placeholder-aspect-ratio: 1019\/1024;\" \/><\/a><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-full\"><a href=\"https:\/\/www.energy.gov\/science\/bes\/basic-energy-sciences\"><img decoding=\"async\" width=\"732\" height=\"725\" data-src=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/DOE-logo.png\" alt=\"Department of Energy Logo\" class=\"wp-image-279 lazyload\" data-srcset=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/DOE-logo.png 732w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/DOE-logo-300x297.png 300w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/DOE-logo-150x150.png 150w\" data-sizes=\"(max-width: 732px) 100vw, 732px\" src=\"data:image\/svg+xml;base64,PHN2ZyB3aWR0aD0iMSIgaGVpZ2h0PSIxIiB4bWxucz0iaHR0cDovL3d3dy53My5vcmcvMjAwMC9zdmciPjwvc3ZnPg==\" style=\"--smush-placeholder-width: 732px; --smush-placeholder-aspect-ratio: 732\/725;\" \/><\/a><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><a href=\"https:\/\/sciences.ucf.edu\/\"><img decoding=\"async\" data-src=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/TheTab_KGrgb_300ppi.png\" alt=\"University of Central Florida Logo\" class=\"wp-image-280 lazyload\" width=\"227\" height=\"306\" data-srcset=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/TheTab_KGrgb_300ppi.png 332w, https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/wp-content\/uploads\/sites\/45\/2023\/07\/TheTab_KGrgb_300ppi-222x300.png 222w\" data-sizes=\"(max-width: 227px) 100vw, 227px\" src=\"data:image\/svg+xml;base64,PHN2ZyB3aWR0aD0iMSIgaGVpZ2h0PSIxIiB4bWxucz0iaHR0cDovL3d3dy53My5vcmcvMjAwMC9zdmciPjwvc3ZnPg==\" style=\"--smush-placeholder-width: 227px; --smush-placeholder-aspect-ratio: 227\/306;\" \/><\/a><\/figure>\n<\/div><\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>A New Science is Born (and won the Nobel Prize!) At the turn of the XX century, transformative advances in laser technology have led to the generation of light pulses with duration as short as few tens of attoseconds (1 as = 10-18 s), which is the characteristic time scale of electrons&#8217; motion in atoms &#8230; <a title=\"Welcome\" class=\"read-more\" href=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/\" aria-label=\"Read more about Welcome\">Read more<\/a><\/p>\n","protected":false},"author":3,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_eb_attr":"","footnotes":"","_links_to":"","_links_to_target":""},"class_list":["post-9","page","type-page","status-publish"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.2 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Welcome - Theoretical Attosecond Science Lab<\/title>\n<meta name=\"description\" content=\"Describes how Luca Argenti&#039;s group contributes to research in theoretical and phenomenological attosecond science\" \/>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/sciences.ucf.edu\/physics\/argenti-lab\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Welcome - 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