{"id":5516,"date":"2023-11-15T12:16:52","date_gmt":"2023-11-15T11:16:52","guid":{"rendered":"https:\/\/www.institut-foton.eu\/?p=5516"},"modified":"2025-04-22T12:27:04","modified_gmt":"2025-04-22T10:27:04","slug":"oror-opto-rf-pour-la-convergence-electronique-photonique","status":"publish","type":"post","link":"https:\/\/www.institut-foton.eu\/en\/oror-opto-rf-pour-la-convergence-electronique-photonique\/","title":{"rendered":"OROR: Opto-RF pour la cOnvergence \u00e9lectRonique photonique"},"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>mars 2023 \u2013 mars 2028<\/p>\n\n\n\n<p>Projet PEPR \u00c9lectronique<\/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-2-1024x390.jpg\" alt=\"\" class=\"wp-image-2440\" style=\"width:158px;height:60px\" srcset=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/ANR-logo-2021-sigle-2-1024x390.jpg 1024w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/ANR-logo-2021-sigle-2-300x114.jpg 300w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/ANR-logo-2021-sigle-2-768x292.jpg 768w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/ANR-logo-2021-sigle-2.jpg 1211w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<figure class=\"wp-block-image size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"227\" height=\"222\" src=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/10\/France-2030.png\" alt=\"\" class=\"wp-image-2470\" style=\"width:96px;height:94px\"\/><\/figure>\n<\/div>\n\n\n\n<p><strong>Doter la France de briques technologiques \u00e0 base de semi-conducteurs III-V pour les futurs syst\u00e8mes \u00e9lectroniques haute fr\u00e9quence<\/strong>.<\/p>\n\n\n\n\n\n\n\n<h2 class=\"wp-block-heading\">Contexte<\/h2>\n\n\n\n<p>Augmenter la fr\u00e9quence des syst\u00e8mes purement \u00e9lectroniques se heurte \u00e0 des limitations d\u2019ordre fondamentale. Introduire la lumi\u00e8re dans ces syst\u00e8mes repousse voire supprime ses limitations. En pratique, cela impose de conf\u00e9rer \u00e0 la lumi\u00e8re utilis\u00e9e des propri\u00e9t\u00e9s spectrales \u00e9quivalentes \u00e0 celles des meilleurs syst\u00e8mes \u00e9lectroniques. Disposer des briques fondamentales, que sont les sources lumineuses, les modulateurs de lumi\u00e8re et les horloges, r\u00e9pondant \u00e0 ces contraintes draconiennes est un d\u00e9fi qui est en passe d\u2019\u00eatre remport\u00e9 en laboratoire. Le projet OROR fait le pari de concevoir tout en les miniaturisant ces trois briques fondamentales avec l\u2019ambition de les int\u00e9grer dans les circuits photoniques du futur. Une telle miniaturisation ultime r\u00e9pond aux enjeux de r\u00e9duction de la consommation \u00e9nerg\u00e9tique mais aussi d\u2019exploitation des technologies optiquehyperfr\u00e9quences dans les syst\u00e8mes \u00e9lectroniques embarqu\u00e9s puis leur diffusion vers le grand public.<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Objectifs<\/h2>\n\n\n\n<p>Des composants optiques pour le transport de l\u2019information dans le domaine RadioFr\u00e9quence (RF):<\/p>\n\n\n\n<ul class=\"puce1 wp-block-list\">\n<li>Les sources laser verticales \u00e0 1,5\u00b5m<\/li>\n\n\n\n<li>Les modulateurs int\u00e9gr\u00e9s III-V sur silicium<\/li>\n\n\n\n<li>Les oscillateurs opto\u00e9lectroniques ultra-int\u00e9gr\u00e9s pour des applications comme la 6G et le g\u00e9o-positionnement<\/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\">26 <\/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>Brian Sinquin, Marc Vallet, Marco Romanelli, Mehdi Alouini. Optoelectronic Oscillator Combining a High-Finesse Cavity and Tilt-Locking Stabilization. <i>IEEE Photonics Technology Letters<\/i>, 2025, 37 (6), pp.321 - 324. <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1109\/lpt.2025.3544428\">&#x27E8;10.1109\/lpt.2025.3544428&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04976326v1\">&#x27E8;hal-04976326&#x27E9;<\/a><\/li><li>Brian Sinquin, Marco Romanelli, Mehdi Alouini, Marc Vallet. Direct-modulation optoelectronic oscillator for optical pulse and frequency comb generation. <i>Journal of the Optical Society of America B<\/i>, 2024, 41 (9), pp.1921. <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1364\/JOSAB.529629\">&#x27E8;10.1364\/JOSAB.529629&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04686127v1\">&#x27E8;hal-04686127&#x27E9;<\/a><\/li><li>Sergio Valenzuela, Pietro Gambardella, Kevin Garello, Olivier Klein, Juan Sierra, et al.. Spintronic materials. <i>Encyclopedia of Condensed Matter Physics<\/i>, 2024, Encyclopedia of Condensed Matter Physics, 2nd edition, 2, pp.159-176. <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1016\/B978-0-323-90800-9.00229-8\">&#x27E8;10.1016\/B978-0-323-90800-9.00229-8&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/cea.hal.science\/cea-05003576v1\">&#x27E8;cea-05003576&#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\">10 documents<\/span><\/h3><div class=\"grp-content\"><ul><li>A. Garnache. Dual-Frequency-Comb generation in a III-V semiconductor laser: Laguerre-Gauss eigenmodes versus degenerate transverse wavefunctions. <i>Frequency Combs France 2025<\/i>, CNRS, Nov 2025, Paris ENS, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05546153v1\">&#x27E8;hal-05546153&#x27E9;<\/a><\/li><li>Mohamed Nadrani, Baptiste Chomet, Adrian Bartolo, Nathan Vigne, Luc Le Gratiet, et al.. Dual-Comb generation in III-V semiconductor external cavity laser: Dual transverse modes versus degenerated cavities solutions. <i>Journ\u00e9es Nationales d'Optique Guid\u00e9e (JNOG 2025)<\/i>, Soci\u00e9t\u00e9 Fran\u00e7aise d'Optique, Jul 2025, S\u00e8te, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05165553v1\">&#x27E8;hal-05165553&#x27E9;<\/a><\/li><li>Brian Sinquin, Marc Vallet, Ludovic Frein, Clara Artur, Marco Romanelli, et al.. Oscillateur opto-\u00e9lectronique int\u00e9grant une cavit\u00e9 ULE asservie par \u00ab tilt-locking \u00bb. <i>Journ\u00e9e du Club Optique Micro-ondes<\/i>, LAAS Toulouse (Laboratoire d'Analyse et d'Architecture des Syst\u00e8mes), Soci\u00e9t\u00e9 Fran\u00e7aise d'Optique, Jun 2025, Toulouse, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05120292v1\">&#x27E8;hal-05120292&#x27E9;<\/a><\/li><li>Arnaud Garnache, Isabelle Sagnes, M. Giudici, Philippe Lalanne, Guillaume Ducournau, et al.. Structured Opto-THz coherent sources based on III-V semiconductor laser technology. <i>Freiburg Infrared Colloquium 2025<\/i>, IAF, Mar 2025, Friburg, Germany. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05546178v1\">&#x27E8;hal-05546178&#x27E9;<\/a><\/li><li>Mohamed Nadrani, Adrian Bartolo, Baptiste Chomet, Im\u00e8ne Si Hadj Mohand, Jean-Paul Guillet, et al.. Emetteurs OPTO-THz structur\u00e9s et coh\u00e9rents par photom\u00e9lange \u00e0 base de technologies III-V. <i>C'Nano, les journ\u00e9es scientifiques annuelles du PEPR \u00e9lectronique 2025<\/i>, CNRS\/CEA, Mar 2025, Paris, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05053849v1\">&#x27E8;hal-05053849&#x27E9;<\/a><\/li><li>M Nadrani, A Bartolo, B Chomet, J.-P Guillet, P.-K Lu, et al.. Source THz coh\u00e9rente accordable bas\u00e9e sur des technologies III-V. <i>Journ\u00e9es Nano, Micro et Opto\u00e9lectronique (JNMO) 2024<\/i>, Oct 2024, S\u00e8te, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04785184v1\">&#x27E8;hal-04785184&#x27E9;<\/a><\/li><li>M. Nadrani, A. Bartolo, B. Chomet, J.P. Guillet, P.K. Lu, et al.. SOURCE THZ COHERENTE ACCORDABLE BASEE SUR DES TECHNOLOGIES III-V. <i>Journ\u00e9es Nano, Micro et Opto\u00e9lectronique, JNMO 2024<\/i>, Oct 2024, S\u00e8te, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04946567v1\">&#x27E8;hal-04946567&#x27E9;<\/a><\/li><li>Brian Sinquin, Marco Romanelli, Mehdi Alouini, Marc Vallet. Direct-Modulation Optoelectronic Oscillator for Optical Pulse and Frequency Comb Generation. <i>Frequency Combs France 2024<\/i>, Jul 2024, Rennes, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05011356v1\">&#x27E8;hal-05011356&#x27E9;<\/a><\/li><li>Mohamed Nadrani, Adri\u00e1n Bartolo, Baptiste Chomet, Jean-Paul Guillet, Ping-Keng Lu, et al.. THz coherent source based on light structuration using III-V semiconductor laser technology. <i>Optique Normandie 2024<\/i>, La Soci\u00e9t\u00e9 Fran\u00e7aise d'Optique, Jul 2024, Rouen, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04592230v1\">&#x27E8;hal-04592230&#x27E9;<\/a><\/li><li>Arnaud Garnache, Mohamed Nadrani, Baptiste Chomet, St\u00e9phane Blin, Isabelle Sagnes, et al.. Structured Opto-THz coherent light sources based on III-V semiconductor laser technology. <i>18th Expert Evaluation and Control of Compound Semiconductor Materials and Technologies<\/i>, Wocsdice-Exmatec, May 2024, Heraklion (Crete Island), Greece. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04800601v1\">&#x27E8;hal-04800601&#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\">7 documents<\/span><\/h3><div class=\"grp-content\"><ul><li>Thomas Perriguey, Marco Romanelli, Hugues Guillet de Chatellus, Quentin Wilmart, Mehdi Alouini. Coherent characterization of an integrated ring resonator based on an acousto-optic frequency-shifting loop. <i>Journ\u00e9es scientifiques du PEPR Electronique 2026<\/i>, Mar 2026, Lyon, France. <a target=\"_blank\" href=\"https:\/\/www.pepr-electronique.fr\/\"><\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05565867v1\">&#x27E8;hal-05565867&#x27E9;<\/a><\/li><li>Eliott Haddad, Cyril Paranthoen, Mathieu Perrin, Mehdi Alouini. Towards compact low noise semiconductor lasers driven by intracavity nonlinearities. <i>Journ\u00e9es scientifiques du PEPR Electronique 2026<\/i>, Mar 2026, Lyon, France. <a target=\"_blank\" href=\"https:\/\/www.pepr-electronique.fr\/\"><\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05570129v1\">&#x27E8;hal-05570129&#x27E9;<\/a><\/li><li>Thomas Perriguey, Hugues Guillet de Chatellus, Goulc'Hen Loas, Quentin Wilmart, Marc Vallet, et al.. Caract\u00e9risation par peigne de fr\u00e9quences d'un r\u00e9sonateur en anneau int\u00e9gr\u00e9. <i>JCOM 2025 - Journ\u00e9e du Club Optique Micro-ondes<\/i>, Jun 2025, Toulouse, France. 2025. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05318352v2\">&#x27E8;hal-05318352v2&#x27E9;<\/a><\/li><li>Thomas Perriguey, Quentin Wilmart, Marc Vallet, Mehdi Alouini, Marco Romanelli. Opto-RF characterization of an integrated ring resonator for the development of optoelectronic oscillators. <i>Journ\u00e9es scientifiques du PEPR Electronique 2025<\/i>, Mar 2025, Paris, France. <a target=\"_blank\" href=\"https:\/\/www.pepr-electronique.fr\/journees-scientifiques-du-pepr-electronique-2025\/#:~:text=Les%20journ%C3%A9es%20scientifiques%202025%20du,du%20congr%C3%A8s%20C'nano%202025.\"><\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05010865v1\">&#x27E8;hal-05010865&#x27E9;<\/a><\/li><li>Mohamed Nadrani, Adri\u00e1n Bartolo, Baptiste Chomet, Jean-Paul Guillet, Ping-Keng Lu, et al.. THZ coherent source based on light structuration using III-V semiconductor laser technology. <i>Optique Normandie 2024<\/i>, Jul 2024, Rouen, France. <a target=\"_blank\" href=\"https:\/\/www.sfoptique.org\/pages\/sfo\/congres-optique\/optique-normandie-2024\/\"><\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04710908v1\">&#x27E8;hal-04710908&#x27E9;<\/a><\/li><li>Mehdi Alouini, L\u00e9opold Virot. Les composants pour les t\u00e9l\u00e9communications - Projet cibl\u00e9 OROR: Opto-RF pour la cOnvergence \u00e9lectRonique photonique. <i>Lancement et premi\u00e8re journ\u00e9e scientifique annuelle du PEPR \u00c9lectronique<\/i>, Mar 2023, Poitiers, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04388460v1\">&#x27E8;hal-04388460&#x27E9;<\/a><\/li><li>Mehdi Alouini, Quentin Wilmart. Les composants pour les t\u00e9l\u00e9communications. Projet cibl\u00e9 OROR. <i>Journ\u00e9es scientifqiues du PEPR Electronique<\/i>, Mar 2023, Poitiers, France. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05010867v1\">&#x27E8;hal-05010867&#x27E9;<\/a><\/li><\/ul><\/div><\/div><br><div class=\"grp-div\"><h3 class=\"wphal-titre-groupe\">Proceedings\/Recueil des communications<span class=\"wphal-nbmetadata\" style=\"margin-left:10px\">5 documents<\/span><\/h3><div class=\"grp-content\"><ul><li>Isabelle Sagnes, Thomas Ernst, Agn\u00e8s Antoine. Journ\u00e9es scientifiques du PEPR \u00c9lectronique 18-20 mars 2026. <i>Journ\u00e9es scientifiques du PEPR \u00e9lectronique<\/i>, Mar 2026, Lyon, France. 2026. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05576886v1\">&#x27E8;hal-05576886&#x27E9;<\/a><\/li><li>Mohamed Nadrani, Baptiste Chomet, Adri\u00e1n Bartolo, Nathan Vigne, Luc Le Gratiet, et al.. Dual-Comb generation in III-V semiconductor laser: Transverse modes versus modeless cavities. <i>CLEO Europe 2025<\/i>, Jun 2025, Munich, Germany. IEEE, pp.1-1, 2025, <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1109\/CLEO\/Europe-EQEC65582.2025.11109387\">&#x27E8;10.1109\/CLEO\/Europe-EQEC65582.2025.11109387&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05057230v1\">&#x27E8;hal-05057230&#x27E9;<\/a><\/li><li>Isabelle Sagnes, Thomas Ernst, Agn\u00e8s Antoine. Journ\u00e9es scientifiques du PEPR \u00c9lectronique 17-21 mars 2025. <i>Journ\u00e9es scientifiques du PEPR \u00e9lectronique<\/i>, Mar 2025, Paris, France. CEA, 2025. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05046672v1\">&#x27E8;hal-05046672&#x27E9;<\/a><\/li><li>Mohamed Nadrani, Baptiste Chomet, Adrian Bartolo, Gr\u00e9goire Beaudoin, Konstantinos Pantzas, et al.. High coherence broadly tunable semiconductor laser: inhibited versus strong non-linear light matter interaction. <i>Semiconductor Lasers and Laser Dynamics XI<\/i>, Apr 2024, Strasbourg, France. SPIE, pp.32, 2024, <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1117\/12.3022556\">&#x27E8;10.1117\/12.3022556&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04695622v1\">&#x27E8;hal-04695622&#x27E9;<\/a><\/li><li>Adrian Bartolo, Mohamed Nadrani, Baptiste Chomet, Alaeddine Abbes, Nathan Vigne, et al.. THz coherent source based on light structuration using III-V semiconductor laser technology. <i>Terahertz Photonics III<\/i>, Apr 2024, Strasbourg, France. SPIE, pp.14, 2024, <a target=\"_blank\" href=\"https:\/\/dx.doi.org\/10.1117\/12.3017105\">&#x27E8;10.1117\/12.3017105&#x27E9;<\/a>. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-04696050v1\">&#x27E8;hal-04696050&#x27E9;<\/a><\/li><\/ul><\/div><\/div><br><div class=\"grp-div\"><h3 class=\"wphal-titre-groupe\">Pr\u00e9-publications, Documents de travail<span class=\"wphal-nbmetadata\" style=\"margin-left:10px\">1 document<\/span><\/h3><div class=\"grp-content\"><ul><li>Gregorio Beltramo, R\u00f3bert Horv\u00e1th, Gr\u00e9goire Beaudoin, Isabelle Sagnes, Sylvain Barbay, et al.. Integrated nano electro-optomechanical spiking neuron. 2026. <a target=\"_blank\" href=\"https:\/\/hal.science\/hal-05520873v1\">&#x27E8;hal-05520873&#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; C2N &#8211; INPHYNI &#8211; CEA-Leti &#8211; IES<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Coordinateur<\/h2>\n\n\n\n<p><a href=\"https:\/\/www.institut-foton.eu\/alouini-mehdi\/\" data-type=\"post\" data-id=\"3565\">Mehdi ALOUINI<\/a> (Foton-DOP)<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Financement<\/h2>\n\n\n\n<p>ANR (?? k\u20ac)<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Voir en ligne<\/h2>\n\n\n\n<figure class=\"wp-block-image size-full\"><a href=\"https:\/\/www.pepr-electronique.fr\/projet_cible_oror\/\"><img loading=\"lazy\" decoding=\"async\" width=\"309\" height=\"171\" src=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/11\/PEPR-e-3.png\" alt=\"\" class=\"wp-image-5518\" srcset=\"https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/11\/PEPR-e-3.png 309w, https:\/\/www.institut-foton.eu\/wp-content\/uploads\/2023\/11\/PEPR-e-3-300x166.png 300w\" sizes=\"auto, (max-width: 309px) 100vw, 309px\" \/><\/a><\/figure>\n","protected":false},"excerpt":{"rendered":"<p>mars 2023 &#8211; mars 2028<br \/>\nCoordinateur iFOTON: Mehdi ALOUINI<\/p>\n","protected":false},"author":9,"featured_media":5519,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"inline_featured_image":false,"footnotes":""},"categories":[25],"tags":[108,110,43],"class_list":["post-5516","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-projets","tag-departement-dop","tag-departement-ohm","tag-lasers-semiconducteurs"],"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\/5516","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=5516"}],"version-history":[{"count":2,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts\/5516\/revisions"}],"predecessor-version":[{"id":6335,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/posts\/5516\/revisions\/6335"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/media\/5519"}],"wp:attachment":[{"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/media?parent=5516"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/categories?post=5516"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.institut-foton.eu\/en\/wp-json\/wp\/v2\/tags?post=5516"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}