Pierre Clad\u00e9 is charg\u00e9 de recherche (CNRS) at Laboratoire Kastler Brossel. He is a specialist in atomic interferometry. He works in particular on the application of this technique to the measurement of the fine structure constant \u03b1. He is also part of the GBAR collaboration aiming at measuring the free fall acceleration of anti-matter in the earth gravity field.<\/p>\n","protected":false},"excerpt":{"rendered":"
Pierre Clad\u00e9 is charg\u00e9 de recherche (CNRS) at Laboratoire Kastler Brossel. He is a specialist in atomic interferometry. He works in particular on the application of this technique to the measurement of the fine structure constant \u03b1. He is also part of the GBAR collaboration aiming at measuring the free fall acceleration of anti-matter in the earth gravity field.<\/p>\n","protected":false},"author":7,"featured_media":2041,"comment_status":"closed","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"_crdt_document":"","_uag_custom_page_level_css":"","_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"_jetpack_memberships_contains_paid_content":false,"footnotes":""},"categories":[47,61],"tags":[],"class_list":["post-2040","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-lecturers-fomo2022","category-pierre-clade"],"jetpack_featured_media_url":"https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?fit=2034%2C475&ssl=1","uagb_featured_image_src":{"full":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?fit=2034%2C475&ssl=1",2034,475,false],"thumbnail":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?resize=150%2C150&ssl=1",150,150,true],"medium":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?fit=300%2C150&ssl=1",300,150,true],"medium_large":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?fit=768%2C384&ssl=1",768,384,true],"large":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?fit=960%2C480&ssl=1",960,480,true],"1536x1536":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?fit=1536%2C359&ssl=1",1536,359,true],"2048x2048":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?fit=2034%2C475&ssl=1",2034,475,true],"ashe-slider-full-thumbnail":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?resize=1080%2C475&ssl=1",1080,540,true],"ashe-full-thumbnail":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?resize=1140%2C266&ssl=1",1140,266,true],"ashe-list-thumbnail":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?resize=300%2C300&ssl=1",300,300,true],"ashe-grid-thumbnail":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?resize=500%2C330&ssl=1",500,330,true],"ashe-single-navigation":["https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2022\/05\/Pierre-Clade.png?resize=75%2C75&ssl=1",75,75,true]},"uagb_author_info":{"display_name":"Atena Zalbeik-Dormayer","author_link":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/author\/zalbeik-dormayer\/"},"uagb_comment_info":0,"uagb_excerpt":"Pierre Clad\u00e9 is charg\u00e9 de recherche (CNRS) at Laboratoire Kastler Brossel. He is a specialist in atomic interferometry. He works in particular on the application of this technique to the measurement of the fine structure constant \u03b1. He is also part of the GBAR collaboration aiming at measuring the free fall acceleration of anti-matter in…","jetpack_sharing_enabled":true,"publishpress_future_action":{"enabled":false,"date":"2026-07-29 18:43:59","action":"category","newStatus":"draft","terms":[],"taxonomy":"category","extraData":[]},"publishpress_future_workflow_manual_trigger":{"enabledWorkflows":[]},"_links":{"self":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/2040","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/users\/7"}],"replies":[{"embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/comments?post=2040"}],"version-history":[{"count":4,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/2040\/revisions"}],"predecessor-version":[{"id":2532,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/2040\/revisions\/2532"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/media\/2041"}],"wp:attachment":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/media?parent=2040"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/categories?post=2040"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/tags?post=2040"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}