{"id":9148,"date":"2023-06-29T08:43:18","date_gmt":"2023-06-29T06:43:18","guid":{"rendered":"https:\/\/fermi.univ-tlse3.fr\/?post_type=tribe_events&#038;p=9148"},"modified":"2023-06-29T08:43:18","modified_gmt":"2023-06-29T06:43:18","slug":"optimal-control-of-quantum-systems-applications-to-the-robust-control-of-bose-einstein-condensates-and-to-quantum-speed-limit-with-piecewise-constant-control-etienne-dionis-lcar-seminar-2","status":"publish","type":"tribe_events","link":"https:\/\/fermi.univ-tlse3.fr\/fr\/home\/event\/optimal-control-of-quantum-systems-applications-to-the-robust-control-of-bose-einstein-condensates-and-to-quantum-speed-limit-with-piecewise-constant-control-etienne-dionis-lcar-seminar-2\/","title":{"rendered":"Optimal control of quantum systems: Applications to the robust control of Bose-Einstein Condensates and to quantum speed limit with piecewise constant control. &#8211; (Etienne Dionis \/ LCAR \/ Seminar). &#8211; 29\/06\/2023, 9H"},"content":{"rendered":"<p><strong><span style=\"font-size: 20px; color: #191970;\">Etienne Dionis<\/span> <\/strong>(Laboratoire Interdisciplinaire Carnot de Bourgogne, Universit\u00e9 de Bourgogne-Franche Comt\u00e9)<\/p>\n<p><span style=\"background-color: #cecece;\">S\u00e9minaire LCAR Jeudi 29 juin, 9H00. &#8211; Nouvelle Salle de conf\u00e9rence, 3R4<\/span><\/p>\n<p><strong>R\u00e9sum\u00e9<\/strong> :<br \/>\nThis presentation will focus on two recent applications of optimal control techniques to quantum<br \/>\nsystems.<\/p>\n<p>In the first part, the goal is to manipulate the motional states of an atomic Bose-Einstein<br \/>\ncondensate (BEC) in a one-dimensional optical lattice. This study is a joint work wit the experi-<br \/>\nmental group of Pr. D. Gu\u00e9ry-Odelin in Toulouse University (France). The protocols operate on<br \/>\nthe momentum comb associated with the lattice through its amplitude and phase [3]. A precise and<br \/>\nversatile control for a wide variety of targets has been demonstrated. However, in order to improve<br \/>\nthe agreement between theory and experiment, it is important to design control processes that are<br \/>\nrobust with respect to experimental uncertainties (Figure 1). One limitation of the experimental<br \/>\nsetup under study is the value of the quasi-momentum which is not exactly zero as assumed in<br \/>\n<strong>[3]<\/strong>. Due to the large dimension of the Hilbert space, numerical algorithms such as GRAPE <strong>[1]<\/strong><br \/>\nhave to be used. In the case of the simultaneous control of an ensemble of systems, we propose<br \/>\na new formulation of GRAPE with a sequential-update of the control. We show numerically the<br \/>\nsuperiority of this sequential approach with respect to the standard one <strong>[2].<\/strong><br \/>\nIn the second part, we apply a recent extension of the Pontryagin Maximum Principle (PMP) <strong>[4]<\/strong><br \/>\nto piecewise constant control. PMP, on which optimal control theory is based, was originally for-<br \/>\nmulated for continuous functions. In practice, experimental implementations resort to piecewise<br \/>\nconstant signals. In<strong> [5]<\/strong>, the authors have mathematically proved that for general non-linear dy-<br \/>\nnamics, the PMP should be modified in a non-trivial way. We have transposed this result to<br \/>\nquantum systems and applied it to the time-optimal control of simple quantum systems with two<br \/>\nlevels (Figure 2). In these systems, we derive exact quantum speed limits accounting for this key<br \/>\nexperimental constraint<strong> [6]<\/strong>. This should be an important step toward understanding the role of<br \/>\ntechnological limitations in the manipulation of quantum systems, a key issue in quantum control.<\/p>\n<p><strong>References<\/strong><br \/>\n<strong>[1] <\/strong>Glaser S. J., Boscain U., Calarco T., Koch C., Kockenberger W., Kosloff R., Kuprov I., Luy<br \/>\nB., Schirmer S., Schulte-Herbr\u00fcggen T., Sugny D. and Wilhelm F. 2015 Eur. Phys. J. D 69,<br \/>\n279<br \/>\n<strong>[2]<\/strong> Dionis E. and Sugny D. 2022 J. Phys. B: At. Mol. Opt. Phys. 55, 184006<br \/>\n<strong>[3]<\/strong> Dupont N., Chatelain G., Gabardos L., Arnal M., Billy J., Peaudecerf B., Sugny D. and<br \/>\nGu\u00e9ry-Odelin D. 2021 PRX Quantum 2, 040303<br \/>\n<strong>[4]<\/strong> Boscain U., Sigalotti M. and Sugny D. 2021 PRX Quantum 2, 030203<br \/>\n<strong>[5]<\/strong> Bourdin L. and Tr\u00e9lat E. 2017 Automatica 79, 273<br \/>\n<strong>[6]<\/strong> Dionis E. and Sugny D. 2023 Physical Review A 107, 032613<\/p>\n<hr \/>\n<p class=\"western\"><code class=\"western\"><div class=\"leaflet-map WPLeafletMap\" style=\"height:300px; width:70%;\"><\/div><script>\nwindow.WPLeafletMapPlugin = window.WPLeafletMapPlugin || [];\nwindow.WPLeafletMapPlugin.push(function WPLeafletMapShortcode() {\/*<script>*\/\nvar baseUrl = atob('aHR0cHM6Ly97c30udGlsZS5vcGVuc3RyZWV0bWFwLm9yZy97en0ve3h9L3t5fS5wbmc=');\nvar base = (!baseUrl && window.MQ) ?\n    window.MQ.mapLayer() : L.tileLayer(baseUrl,\n        L.Util.extend({}, {\n            detectRetina: 0,\n        },\n        {\"subdomains\":\"abc\",\"noWrap\":false,\"maxZoom\":18}        )\n    );\n    var options = L.Util.extend({}, {\n        layers: [base],\n        attributionControl: false\n    },\n    {\"zoomControl\":true,\"scrollWheelZoom\":true,\"doubleClickZoom\":true,\"fitBounds\":true,\"minZoom\":9,\"maxZoom\":18,\"maxBounds\":null,\"attribution\":\"<a href=\\\"http:\\\/\\\/leafletjs.com\\\" title=\\\"Une biblioth\\u00e8que JS pour des cartes interactives\\\">Leaflet<\\\/a>; \\u00a9 <a href=\\\"http:\\\/\\\/www.openstreetmap.org\\\/copyright\\\">OpenStreetMap<\\\/a> contributeurs\"},\n    {});\nwindow.WPLeafletMapPlugin.createMap(options).setView([43.560830727361,1.4672373725804],16);window.WPLeafletMapPlugin.createScale({});});<\/script><\/code><\/p>\n<p class=\"western\"><code class=\"western\"><script>\nwindow.WPLeafletMapPlugin = window.WPLeafletMapPlugin || [];\nwindow.WPLeafletMapPlugin.push(function WPLeafletMarkerShortcode() {\/*<script>*\/\nvar map = window.WPLeafletMapPlugin.getCurrentMap();\nvar group = window.WPLeafletMapPlugin.getCurrentGroup();\nvar marker_options = window.WPLeafletMapPlugin.getIconOptions({});\nvar marker = L.marker(\n    [0,0],\n    marker_options\n);\nvar is_image = map.is_image_map;\n    marker.setLatLng( map.getCenter() );\nif (marker_options.draggable) {\n    marker.on('dragend', function () {\n        var latlng = this.getLatLng();\n        var lat = latlng.lat;\n        var lng = latlng.lng;\n        if (is_image) {\n            console.log('leaflet-marker y=' + lat + ' x=' + lng);\n        } else {\n            console.log('leaflet-marker lat=' + lat + ' lng=' + lng);\n        }\n    });\n}\nmarker.addTo( group );\nmarker.bindPopup(window.WPLeafletMapPlugin.unescape('&lt;strong class=&quot;&quot;&gt;Salle de conf\u00e9rence&lt;\/strong&gt; (- B\u00e2timent 3R4)'));window.WPLeafletMapPlugin.markers.push( marker );\n        });<\/script><\/code><\/p>\n","protected":false},"excerpt":{"rendered":"<p>This presentation will focus on two recent applications of optimal control techniques to quantum systems.<\/p>\n","protected":false},"author":5,"featured_media":0,"template":"","meta":{"neve_meta_sidebar":"","neve_meta_container":"","neve_meta_enable_content_width":"","neve_meta_content_width":0,"neve_meta_title_alignment":"","neve_meta_author_avatar":"","neve_post_elements_order":"","neve_meta_disable_header":"","neve_meta_disable_footer":"","neve_meta_disable_title":"","_tribe_events_status":"","_tribe_events_status_reason":"","footnotes":""},"tags":[],"tribe_events_cat":[48,309,233],"class_list":["post-9148","tribe_events","type-tribe_events","status-publish","hentry","tribe_events_cat-events","tribe_events_cat-lcar","tribe_events_cat-seminars","cat_events","cat_lcar","cat_seminars"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v28.5 - 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