{"id":881,"date":"2021-04-20T09:00:49","date_gmt":"2021-04-20T09:00:49","guid":{"rendered":"https:\/\/s-baxit.optimato.eu\/?p=881"},"modified":"2023-02-22T13:44:15","modified_gmt":"2023-02-22T13:44:15","slug":"ptychography-for-xfel-pulse-characterization","status":"publish","type":"post","link":"https:\/\/s-baxit.optimato.eu\/index.php\/2021\/04\/20\/ptychography-for-xfel-pulse-characterization\/","title":{"rendered":"Ptychography for XFEL pulse characterization"},"content":{"rendered":"<p>In a new paper published last week<span class=\"footnote_referrer\"><a role=\"button\" tabindex=\"0\" onclick=\"footnote_moveToReference_881_1('footnote_plugin_reference_881_1_1');\" onkeypress=\"footnote_moveToReference_881_1('footnote_plugin_reference_881_1_1');\" ><sup id=\"footnote_plugin_tooltip_881_1_1\" class=\"footnote_plugin_tooltip_text\">1<\/sup><\/a><span id=\"footnote_plugin_tooltip_text_881_1_1\" class=\"footnote_tooltip\"><a href=https:\/\/doi.org\/10.1364\/optica.416655>Daurer2021<\/a><\/span><\/span><script type=\"text\/javascript\"> jQuery('#footnote_plugin_tooltip_881_1_1').tooltip({ tip: '#footnote_plugin_tooltip_text_881_1_1', tipClass: 'footnote_tooltip', effect: 'fade', predelay: 0, fadeInSpeed: 200, delay: 400, fadeOutSpeed: 200, position: 'top center', relative: true, offset: [-7, 0], });<\/script>, we show how ptychography can be used to characterize the extremely short and powerful X-ray pulses generated at the Linac Coherent Light Source (LCLS, SLAC Stanford, USA), one of the few X-ray free-electron lasers operating in the world. The work is the result of a broad collaboration, including present and former members of the Maia group (Uppsala University, Sweden) and the Loh group (National University of Singapore).<\/p>\n<p>This paper follows a previous work<span class=\"footnote_referrer\"><a role=\"button\" tabindex=\"0\" onclick=\"footnote_moveToReference_881_1('footnote_plugin_reference_881_1_2');\" onkeypress=\"footnote_moveToReference_881_1('footnote_plugin_reference_881_1_2');\" ><sup id=\"footnote_plugin_tooltip_881_1_2\" class=\"footnote_plugin_tooltip_text\">2<\/sup><\/a><span id=\"footnote_plugin_tooltip_text_881_1_2\" class=\"footnote_tooltip\"><a href=http:\/\/doi.org\/10.1107\/s1600576720006913>Sala2020<\/a><\/span><\/span><script type=\"text\/javascript\"> jQuery('#footnote_plugin_tooltip_881_1_2').tooltip({ tip: '#footnote_plugin_tooltip_text_881_1_2', tipClass: 'footnote_tooltip', effect: 'fade', predelay: 0, fadeInSpeed: 200, delay: 400, fadeOutSpeed: 200, position: 'top center', relative: true, offset: [-7, 0], });<\/script> that was conducted with many of the same collaborators to characterize the X-ray pulses generated at FERMI, Italy&#8217;s very own free-electron lasers, also hosted here in Trieste.<\/p>\n<div class=\"speaker-mute footnotes_reference_container\"> <div class=\"footnote_container_prepare\"><p><span role=\"button\" tabindex=\"0\" class=\"footnote_reference_container_label pointer\" onclick=\"footnote_expand_collapse_reference_container_881_1();\">References<\/span><span role=\"button\" tabindex=\"0\" class=\"footnote_reference_container_collapse_button\" style=\"display: none;\" onclick=\"footnote_expand_collapse_reference_container_881_1();\">[<a id=\"footnote_reference_container_collapse_button_881_1\">+<\/a>]<\/span><\/p><\/div> <div id=\"footnote_references_container_881_1\" style=\"\"><table class=\"footnotes_table footnote-reference-container\"><caption class=\"accessibility\">References<\/caption> <tbody> \r\n\r\n<tr class=\"footnotes_plugin_reference_row\"> <th scope=\"row\" class=\"footnote_plugin_index_combi pointer\"  onclick=\"footnote_moveToAnchor_881_1('footnote_plugin_tooltip_881_1_1');\"><a id=\"footnote_plugin_reference_881_1_1\" class=\"footnote_backlink\"><span class=\"footnote_index_arrow\">&#8593;<\/span>1<\/a><\/th> <td class=\"footnote_plugin_text\">B. J. Daurer, S. Sala, M. F. Hantke, H. K. N. Reddy, J. Bielecki, Z. Shen, C. Nettelblad, M. Svenda, T. Ekeberg; G. A. Carini, P. Hart; T. Osipov; A. Aquila, N. D. Loh, F. R. N. C. Maia and P. Thibault, <a href=https:\/\/doi.org\/10.1364\/optica.416655>Ptychographic wavefront characterization for single-particle imaging at x-ray lasers<\/a>, <b>Optica<\/b> (2021)<\/td><\/tr>\r\n\r\n<tr class=\"footnotes_plugin_reference_row\"> <th scope=\"row\" class=\"footnote_plugin_index_combi pointer\"  onclick=\"footnote_moveToAnchor_881_1('footnote_plugin_tooltip_881_1_2');\"><a id=\"footnote_plugin_reference_881_1_2\" class=\"footnote_backlink\"><span class=\"footnote_index_arrow\">&#8593;<\/span>2<\/a><\/th> <td class=\"footnote_plugin_text\">S. Sala, B. J. Daurer, M. Odstrcil, F. Capotondi, E. Pedersoli, M. F. Hantke, M. Manfredda, N. D. Loh, P. Thibault and F. R. N. C. Maia, <a href=http:\/\/doi.org\/10.1107\/s1600576720006913>Pulse-to-pulse wavefront sensing at free-electron lasers using ptychography<\/a>, <b>J. Appl. Crystallogr.<\/b> (2020)<\/td><\/tr>\r\n\r\n <\/tbody> <\/table> <\/div><\/div><script type=\"text\/javascript\"> function footnote_expand_reference_container_881_1() { jQuery('#footnote_references_container_881_1').show(); jQuery('#footnote_reference_container_collapse_button_881_1').text('\u2212'); } function footnote_collapse_reference_container_881_1() { jQuery('#footnote_references_container_881_1').hide(); jQuery('#footnote_reference_container_collapse_button_881_1').text('+'); } function footnote_expand_collapse_reference_container_881_1() { if (jQuery('#footnote_references_container_881_1').is(':hidden')) { footnote_expand_reference_container_881_1(); } else { footnote_collapse_reference_container_881_1(); } } function footnote_moveToReference_881_1(p_str_TargetID) { footnote_expand_reference_container_881_1(); var l_obj_Target = jQuery('#' + p_str_TargetID); if (l_obj_Target.length) { jQuery( 'html, body' ).delay( 0 ); jQuery('html, body').animate({ scrollTop: l_obj_Target.offset().top - window.innerHeight * 0.2 }, 380); } } function footnote_moveToAnchor_881_1(p_str_TargetID) { footnote_expand_reference_container_881_1(); var l_obj_Target = jQuery('#' + p_str_TargetID); if (l_obj_Target.length) { jQuery( 'html, body' ).delay( 0 ); jQuery('html, body').animate({ scrollTop: l_obj_Target.offset().top - window.innerHeight * 0.2 }, 380); } }<\/script>","protected":false},"excerpt":{"rendered":"<p>In a new paper published last week, we show how ptychography can be used to characterize the extremely short and powerful X-ray pulses generated at the Linac Coherent Light Source (LCLS, SLAC Stanford, USA), one of the few X-ray free-electron lasers operating in the world. The work is the result of a broad collaboration, including&hellip; <a class=\"more-link\" href=\"https:\/\/s-baxit.optimato.eu\/index.php\/2021\/04\/20\/ptychography-for-xfel-pulse-characterization\/\">Continue reading <span class=\"screen-reader-text\">Ptychography for XFEL pulse characterization<\/span><\/a><\/p>\n","protected":false},"author":2,"featured_media":882,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[10,109],"tags":[113,114,115],"class_list":["post-881","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-news","category-publication","tag-ptychography","tag-ptypy","tag-xfel","entry"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v25.9 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>Ptychography for XFEL pulse characterization - S-BaXIT<\/title>\n<meta name=\"description\" content=\"In a new paper, we show how ptychography can be used to characterize the short and powerful X-ray pulses generated at the LCLS free-electron laser.\" \/>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/s-baxit.optimato.eu\/index.php\/2021\/04\/20\/ptychography-for-xfel-pulse-characterization\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Ptychography for XFEL pulse characterization - 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