{"id":5524,"date":"2023-08-01T12:36:21","date_gmt":"2023-08-01T10:36:21","guid":{"rendered":"https:\/\/www.institut-foton.eu\/?p=5524"},"modified":"2025-04-22T12:33:58","modified_gmt":"2025-04-22T10:33:58","slug":"teldot-composants-a-base-de-boites-quantiques-pour-applications-en-telecommunications","status":"publish","type":"post","link":"https:\/\/www.institut-foton.eu\/en\/teldot-composants-a-base-de-boites-quantiques-pour-applications-en-telecommunications\/","title":{"rendered":"TELDOT: Composants \u00e0 base de boites quantiques pour applications en t\u00e9l\u00e9communications"},"content":{"rendered":"\n<div class=\"wp-block-group is-nowrap is-layout-flex wp-container-core-group-is-layout-6c531013 wp-block-group-is-layout-flex\">\n<div class=\"wp-block-group is-vertical is-layout-flex wp-container-core-group-is-layout-fe9cc265 wp-block-group-is-layout-flex\">\n<p>d\u00e9cembre 2009 \u2013 mai 2013<\/p>\n\n\n\n<p>Projet ANR-09-VERS-001 (ANR)<\/p>\n<\/div>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<figure class=\"wp-block-image size-large is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"390\" src=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/ANR-logo-2021-sigle-1024x390.jpg\" alt=\"\" class=\"wp-image-1364\" style=\"width:218px;height:72px\" srcset=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/ANR-logo-2021-sigle-1024x390.jpg 1024w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/ANR-logo-2021-sigle-300x114.jpg 300w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/ANR-logo-2021-sigle-768x292.jpg 768w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/ANR-logo-2021-sigle.jpg 1211w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n<\/div>\n\n\n\n<p>Des effets non lin\u00e9aires exalt\u00e9s ont r\u00e9cemment permis de d\u00e9velopper des lasers \u00e0 blocage de modes \u00e0 une seule section \u00e0 base de boites quantiques (BQs) sur substrat InP, sans avoir recours \u00e0 un absorbant saturable.<br>L\u2019objectif du projet TELDOT est d\u2019exploiter compl\u00e8tement le potentiel de ce type de lasers comme nouvelles sources pr\u00e9sentant une solution innovante pour les r\u00e9seaux d\u2019acc\u00e8s et m\u00e9tropolitains.<\/p>\n\n\n\n\n\n\n\n<h2 class=\"wp-block-heading\">Contexte<\/h2>\n\n\n\n<p>Pour faire face \u00e0 l\u2019explosion du trafic internet, il est n\u00e9cessaire de <strong>d\u00e9velopper des r\u00e9seaux optiques \u00e0 haut d\u00e9bit et large bande passante<\/strong>. L\u2019un des enjeux repose sur la capacit\u00e9 \u00e0 <strong>r\u00e9aliser des composants optiques bas co\u00fbts, de faible encombrement et \u00e0 faible consommation tout en am\u00e9liorant leurs performances<\/strong>. Depuis une dizaine d\u2019ann\u00e9es, les lasers \u00e0 base de bo\u00eetes quantiques (BQs) suscitent un fort int\u00e9r\u00eat en raison de leurs propri\u00e9t\u00e9s th\u00e9oriques remarquables r\u00e9sultant du confinement tridimensionnel des porteurs de charges. Ces lasers \u00e0 base de nanostructures pr\u00e9sentent certaines performances sup\u00e9rieures \u00e0 celles des lasers \u00e0 puits quantiques \u00e0 un co\u00fbt plus faible (e.g. un courant de seuil plus faible, une \u00e9lectronique de contr\u00f4le simplifi\u00e9e, \u2026). <strong>Des effets non lin\u00e9aires exalt\u00e9s ont r\u00e9cemment permis de d\u00e9velopper des lasers \u00e0 blocage de modes \u00e0 une seule section \u00e0 base de BQs sur substrat InP<\/strong>, sans avoir recours \u00e0 un absorbant saturable.<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Objectifs<\/h2>\n\n\n\n<p>L\u2019objectif de Teldot est d\u2019exploiter compl\u00e8tement le potentiel de ce type de lasers comme <strong>nouvelles sources pr\u00e9sentant une solution innovante pour les r\u00e9seaux d\u2019acc\u00e8s et m\u00e9tropolitains<\/strong>. Ce projet inclut :<\/p>\n\n\n\n<ul class=\"puce1 wp-block-list\">\n<li>Le <strong>d\u00e9veloppement de lasers \u00e0 blocage de mode<\/strong> \u00e0 base de BQs pr\u00e9sentant un faible bruit pour la g\u00e9n\u00e9ration de peignes de fr\u00e9quences (16-32 canaux) <strong>\u00e0 1,3 \u00b5m et 1,55 \u00b5m compatibles pour la transmission \u00e0 10 Gbit\/s<\/strong><\/li>\n\n\n\n<li>Le d\u00e9veloppement de lasers \u00e0 blocage de mode \u00e0 base de BQs pr\u00e9sentant un faible bruit et une fr\u00e9quence de r\u00e9p\u00e9tition de 60 GHz pour des applications de type radio sur fibre<\/li>\n\n\n\n<li>La mise en \u0153uvre de ces sources dans des plateformes d\u2019exp\u00e9rimentation par un partenaire t\u00e9l\u00e9com (FT-Orange) et partenaires acad\u00e9miques : Fibre chez l\u2019abonn\u00e9 : r\u00e9seaux de type passif WDM et r\u00e9seaux m\u00e9tropolitains exploitant ces peignes de fr\u00e9quences Radio sur fibre avec des signaux multi-gigabit\/s<\/li>\n<\/ul>\n\n\n\n<h2 class=\"wp-block-heading\">Production scientifique<\/h2>\n\n\n<div id=\"wphal-content\"><div id=\"meta\">\n        <div class=\"display\" id=\"wphal-contact\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">Contact<\/h3>\n\n            <ul id=\"wphal-cont\" style=\"list-style-type: none\"><\/ul>\n        <\/div>\n        <div class=\"display\" id=\"wphal-disciplines\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">Disciplines<\/h3><\/div>\n        <div class=\"display\" id=\"wphal-keywords\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">Mots-clefs<\/h3><\/div>\n        <div class=\"display\" id=\"wphal-auteurs\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">Auteurs<\/h3><\/div>\n        <div class=\"display\" id=\"wphal-affiliated\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">Auteurs de la structure<\/h3><\/div>\n        <div class=\"display\" id=\"wphal-revues\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">Revues<\/h3><\/div>\n        <div class=\"display\" id=\"wphal-annees\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">Ann\u00e9e de production<\/h3><\/div>\n        <div class=\"display\" id=\"wphal-insts\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">Institutions<\/h3><\/div>\n       <div class=\"display\" id=\"wphal-labs\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">Laboratoires<\/h3><\/div>\n       <div class=\"display\" id=\"wphal-depts\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">D\u00e9partements<\/h3><\/div>\n       <div class=\"display\" id=\"wphal-equipes\" style=\"display: none\">\n            <h3 class=\"wphal-titre\">\u00c9quipes de recherche<\/h3><\/div>\n    <div class=\"display\" id=\"publications\"><div class=\"counter-doc\"><span class=\"wphal-nbtot\">15 <\/span>documents<\/div><br><div class=\"grp-div\"><h3 class=\"wphal-titre-groupe\">Articles dans une revue<span class=\"wphal-nbmetadata\" style=\"margin-left:10px\">3 documents<\/span><\/h3><div class=\"grp-content\"><ul><li>Kamil Klaime, Cosimo Calo, Rozenn Piron, Cyril Paranthoen, Dame Thiam, et al.. 23 and 39 GHz low phase noise monosection InAs\/InP (113)B quantum dots mode-locked lasers. <i>Optics Express<\/i>, 2013, 21 (23), pp.29000-29005. <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1364\/OE.21.029000\">&#x27E8;10.1364\/OE.21.029000&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-01167812v1\">&#x27E8;hal-01167812&#x27E9;<\/a><\/li><li>Habeb Rzaigui, Julien Poette, Beatrice Cabon, Friederike Brendel, Ramin Khayatzadeh. Optical Heterodyning for Reduction of Chromatic Dispersion Sensitivity in 60 GHz Mode-Locked Laser Systems. <i>Journal of Lightwave Technology<\/i>, 2013, 31 (17), pp.2955-2960. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-01954334v1\">&#x27E8;hal-01954334&#x27E9;<\/a><\/li><li>B. Cabon, F. Brendel, J. Poette. Comparisons of system architectures for microwave-photonics transmissions at 60\u00a0GHz. <i>Annals of Telecommunications - annales des t\u00e9l\u00e9communications<\/i>, 2013, 68 (1-2), pp.41-48. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-01954344v1\">&#x27E8;hal-01954344&#x27E9;<\/a><\/li><\/ul><\/div><\/div><br><div class=\"grp-div\"><h3 class=\"wphal-titre-groupe\">Communications dans un congr\u00e8s<span class=\"wphal-nbmetadata\" style=\"margin-left:10px\">6 documents<\/span><\/h3><div class=\"grp-content\"><ul><li>Mohamed E Chaibi, Laurent Bramerie, S\u00e9bastien Lobo, Christophe Peucheret. Mitigation of mode partition noise in quantum-dash Fabry- Perot mode-locked lasers using Manchester encoding. <i>42nd European Conference on Optical Communication (ECOC 2016)<\/i>, Sep 2016, Duesseldorf, Germany. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-01461201v1\">&#x27E8;hal-01461201&#x27E9;<\/a><\/li><li>Mathilde Gay, Arthur O'Hare, Laurent Bramerie, Zhenyu Hao, Schadrac Fresnel, et al.. Single quantum dash mode-locked laser as a comb-generator in four-channel 112 Gbit\/s WDM transmission. <i>Optical Fiber Communication 2014 (OFC 2014)<\/i>, Mar 2014, San Francisco, CA, United States. pp.Tu2H.5, <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1364\/OFC.2014.Tu2H.5\">&#x27E8;10.1364\/OFC.2014.Tu2H.5&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-00966203v1\">&#x27E8;hal-00966203&#x27E9;<\/a><\/li><li>Kamil Klaime, Rozenn Piron, Frederic Grillot, Madhoussoudhana Dontabactouny, Slimane Loualiche, et al.. Systematic investigation of the temperature behavior of InAs\/InP quantum nanostructure passively mode-locked lasers. <i>SPIE Photonics West - OPTO 2013<\/i>, Feb 2013, San Francisco, United States. pp.863407, <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1117\/12.2005244\">&#x27E8;10.1117\/12.2005244&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-01167250v1\">&#x27E8;hal-01167250&#x27E9;<\/a><\/li><li>Kamil Klaime, Rozenn Piron, Cyril Parantho\u00ebn, Thomas Batte, Frederic Grillot, et al.. High Frequency Quantum Dots Mode Locked Laser for Telecommunication Applications. <i>European Semiconductor Laser Workshop (ESLW 2012)<\/i>, Sep 2012, Brussels, Belgium. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-00806320v1\">&#x27E8;hal-00806320&#x27E9;<\/a><\/li><li>Kamil Klaime, Rozenn Piron, Cyril Paranthoen, Thomas Batte, Frederic Grillot, et al.. 20 GHz to 83 GHz single section InAs\/InP quantum dot mode-locked lasers grown on (001) misoriented substrate. <i>24th International Conference on Indium Phosphide and Related Materials (IPRM 2012)<\/i>, Aug 2012, Santa Barbara, United States. pp.181-184, <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1109\/ICIPRM.2012.6403352\">&#x27E8;10.1109\/ICIPRM.2012.6403352&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-00726881v1\">&#x27E8;hal-00726881&#x27E9;<\/a><\/li><li>Cosimo Calo, Kamel Merghem, Ricardo Rosales, Anthony Martinez, Abderrahim Ramdane, et al.. Self Pulsation in Quantum Dot lasers operating at 1.55 \u03bcm based on (311)B substrates. <i>International Nano-Optoelectronics Workshop 2012<\/i>, Aug 2012, Berkeley, United States. pp.1. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-00726928v1\">&#x27E8;hal-00726928&#x27E9;<\/a><\/li><\/ul><\/div><\/div><br><div class=\"grp-div\"><h3 class=\"wphal-titre-groupe\">Poster de conf\u00e9rence<span class=\"wphal-nbmetadata\" style=\"margin-left:10px\">4 documents<\/span><\/h3><div class=\"grp-content\"><ul><li>Kamil Klaime, Dame Thiam, Rozenn Piron, Cyril Paranthoen, Thomas Batte, et al.. Single and Double Section InAs Quantum Dots Mode\u2010Locked Laser Elaborated on Misoriented (001) InP Substrate. <i>International Symposium on Physics and Applications of Laser Dynamics 2013 (IS-PALD 2013)<\/i>, Oct 2013, Paris, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-01165707v1\">&#x27E8;hal-01165707&#x27E9;<\/a><\/li><li>Kamil Klaime, Rozenn Piron, Dame Thiam, Cyril Paranthoen, Olivier Dehaese, et al.. Lasers \u00e0 blocage de modes bi-section \u00e0 base de boites quantiques InAs sur InP (001) d\u00e9sorient\u00e9 \u00e9mettant \u00e0 1,64 \u00b5m \u00e0 des taux de r\u00e9p\u00e9titions de 22,6 GHz. <i>Optique Paris XIII - 33\u00e8 Journ\u00e9es Nationales d'Optique Guid\u00e9e (JNOG'33)<\/i>, Jul 2013, Villetaneuse, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-01167850v1\">&#x27E8;hal-01167850&#x27E9;<\/a><\/li><li>Kamil Klaime, Rozenn Piron, Dame Thiam, Cyril Paranthoen, Nicolas Chevalier, et al.. Lasers \u00e0 blocage de modes mono-section \u00e0 base de boites quantiques InAs sur InP \u00e9mettant dans la bande L \u00e0 un taux de r\u00e9p\u00e9tition de 102 GHz. <i>Journ\u00e9es Bo\u00eetes Quantiques 2013 (JBQ 2013)<\/i>, Jun 2013, Paris, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-01165712v1\">&#x27E8;hal-01165712&#x27E9;<\/a><\/li><li>Kamil Klaime, Cosimo Calo, Rozenn Piron, Cyril Paranthoen, Dame Thiam, et al.. InAs\/InP quantum dot mode-locked lasers grown on (113)B InP substrate. <i>Compound Semiconductor Week 2013 - 25th International Conference on Indium Phosphide and Related Materials (IPRM 2013)<\/i>, May 2013, Kobe, Japan. IEEE (ISBN: 978-1-4673-6130-9), IEEE Xplore Digital Library, pp.1-2, 2013, International Conference on Indium Phosphide and Related Materials (IPRM), 2013. <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1109\/ICIPRM.2013.6562595\">&#x27E8;10.1109\/ICIPRM.2013.6562595&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-01167841v1\">&#x27E8;hal-01167841&#x27E9;<\/a><\/li><\/ul><\/div><\/div><br><div class=\"grp-div\"><h3 class=\"wphal-titre-groupe\">Autres publications<span class=\"wphal-nbmetadata\" style=\"margin-left:10px\">2 documents<\/span><\/h3><div class=\"grp-content\"><ul><li>Fatiha Boujdaine, Nazim Agoulmine. Infrastructures mat\u00e9rielles et logicielles (r\u00e9seaux de communication, traitement et stockage) pour la soci\u00e9t\u00e9 num\u00e9rique. 2016. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-03413135v1\">&#x27E8;hal-03413135&#x27E9;<\/a><\/li><li>Julien Haccoun, Didier Theron. Les nanotechnologies : un nouveau paradigme. 2012. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-03413001v1\">&#x27E8;hal-03413001&#x27E9;<\/a><\/li><\/ul><\/div><\/div><br><\/div>\n    <\/div>\n<\/div><div class=\"wphal-footer\"><p style=\"color:#B3B2B0\">Documents r\u00e9cup\u00e9r\u00e9s de l'archive ouverte HAL&nbsp;<a href=\"https:\/\/hal.science\/\" target=\"_blank\"><img decoding=\"async\" alt=\"logo\" src=\"https:\/\/www.institut-foton.eu\/wp-content\/plugins\/hal\/img\/logo-hal.png\" style=\"width:90px\"><\/a><\/p><\/div>\n\n\n\n<h2 class=\"wp-block-heading\">Partenaires<\/h2>\n\n\n\n<p>FOTON &#8211; <a href=\"http:\/\/www.orange.com\/fr\/accueil\">Orange Labs<\/a> \u2013 <a href=\"http:\/\/www.lpn.cnrs.fr\/fr\/Commun\/\">CNRS LPN<\/a> \u2013 <a href=\"http:\/\/www.3-5lab.fr\/\">III-V Lab<\/a> \u2013 <a href=\"http:\/\/imep-lahc.grenoble-inp.fr\/accueil\/laboratoire-de-microelectronique-electromagnetisme-photonique-et-micro-ondes-416667.kjsp?RH=IMEP_EN\">IMEP-LAHC<\/a><a href=\"http:\/\/lpn.epfl.ch\/\">L<\/a><\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Coordinateur<\/h2>\n\n\n\n<p>Fran\u00e7ois Lelarge (<a href=\"http:\/\/www.3-5lab.fr\/\">III-V Lab<\/a>)<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Financement<\/h2>\n\n\n\n<p>ANR VERSO \u2013 P\u00f4le I&amp;R<\/p>\n","protected":false},"excerpt":{"rendered":"<p>d\u00e9cembre 2009 \u2013 mai 2013<\/p>\n","protected":false},"author":9,"featured_media":5526,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"inline_featured_image":false,"footnotes":""},"categories":[25],"tags":[110],"class_list":["post-5524","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-projets","tag-departement-ohm"],"translation":{"provider":"WPGlobus","version":"3.0.2","language":"en","enabled_languages":["fr","en"],"languages":{"fr":{"title":true,"content":true,"excerpt":true},"en":{"title":false,"content":false,"excerpt":false}}},"_links":{"self":[{"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts\/5524","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/users\/9"}],"replies":[{"embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/comments?post=5524"}],"version-history":[{"count":1,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts\/5524\/revisions"}],"predecessor-version":[{"id":5527,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts\/5524\/revisions\/5527"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/media\/5526"}],"wp:attachment":[{"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/media?parent=5524"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/categories?post=5524"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/tags?post=5524"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}