{"id":1329,"date":"2024-08-29T14:23:39","date_gmt":"2024-08-29T12:23:39","guid":{"rendered":"http:\/\/nanophononics.eu\/?page_id=1329"},"modified":"2024-08-30T10:31:25","modified_gmt":"2024-08-30T08:31:25","slug":"2019-2","status":"publish","type":"page","link":"http:\/\/nanophononics.eu\/?page_id=1329","title":{"rendered":"2019"},"content":{"rendered":"\n<h4><span style=\"color: #008000;\"><a href=\"https:\/\/journals.aps.org\/prb\/abstract\/10.1103\/PhysRevB.100.085430\">Phonon engineering with superlattices: generalized nanomechanical potentials<\/a><br \/><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">O. Ortiz, M. Esmann, N. D. Lanzillotti-Kimura<br \/>Phys. Rev. B\u00a0<strong>100<\/strong>, 085430, 2019 <em style=\"color: #008000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><img decoding=\"async\" loading=\"lazy\" class=\"alignnone wp-image-269\" src=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-192x300.png\" alt=\"\" width=\"12\" height=\"19\" srcset=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-192x300.png 192w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-100x157.png 100w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-150x235.png 150w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_.png 200w\" sizes=\"(max-width: 12px) 100vw, 12px\" \/><\/span><\/em><\/span><\/span><\/h4>\n<p>\u00a0<\/p>\n<h4><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><em><img decoding=\"async\" loading=\"lazy\" class=\"alignright wp-image-879\" src=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/cover-optica-6-7_page-0001-232x300.jpg\" alt=\"\" width=\"200\" height=\"259\" srcset=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/cover-optica-6-7_page-0001-232x300.jpg 232w, http:\/\/nanophononics.eu\/wp-content\/uploads\/cover-optica-6-7_page-0001-791x1024.jpg 791w, http:\/\/nanophononics.eu\/wp-content\/uploads\/cover-optica-6-7_page-0001-768x994.jpg 768w, http:\/\/nanophononics.eu\/wp-content\/uploads\/cover-optica-6-7_page-0001-1187x1536.jpg 1187w, http:\/\/nanophononics.eu\/wp-content\/uploads\/cover-optica-6-7_page-0001.jpg 1275w\" sizes=\"(max-width: 200px) 100vw, 200px\" \/><\/em><\/span><\/h4>\n<h4><span style=\"color: #008000;\"><a href=\"https:\/\/doi.org\/10.1364\/OPTICA.6.000854\">Brillouin scattering in hybrid optophononic Bragg micropillar resonators at 300GHz<\/a><br \/><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">M. Esmann, F. R. Lamberti, A. Harouri, L. Lanco, I. Sagnes, I. Favero, G. Aubin, <\/span><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">C. Gomez-Carbonell, A. Lemaitre, O. Krebs, P. Senellart, N. D. Lanzillotti-Kimura<\/span><\/span><br \/><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\">Optica <strong>6<\/strong>, 854, 2019 <\/span><a style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 13.3333px;\" href=\"https:\/\/doi.org\/10.1063\/1.5082728\"><em style=\"color: #008000;\"><span style=\"font-size: 10pt;\"><img decoding=\"async\" loading=\"lazy\" class=\"alignnone wp-image-269\" src=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-192x300.png\" alt=\"\" width=\"12\" height=\"19\" srcset=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-192x300.png 192w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-100x157.png 100w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-150x235.png 150w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_.png 200w\" sizes=\"(max-width: 12px) 100vw, 12px\" \/><\/span><\/em><\/a><\/h4>\n<p>\u00a0<\/p>\n<h4><span style=\"color: #008000;\"><a href=\"https:\/\/doi.org\/10.1063\/1.5082728\">Coherent generation and detection of acoustic phonons in topological nanocavities<\/a><br \/><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">G. Arregui, O. Ortiz, M. Esmann, C. M. Sotomayor-Torres, C. Gomez-Carbonell, O. Mauguin, B. Perrin, A. Lemaitre, P. D. Garc\u00eda, N. D. Lanzillotti-Kimura<br \/>APL Photonics <strong>4<\/strong>, 030805, 2019<a style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 13.3333px;\" href=\"https:\/\/doi.org\/10.1063\/1.5082728\"><em style=\"color: #008000;\"><span style=\"font-size: 10pt;\"><img decoding=\"async\" loading=\"lazy\" class=\"alignnone wp-image-269\" src=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-192x300.png\" alt=\"\" width=\"12\" height=\"19\" srcset=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-192x300.png 192w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-100x157.png 100w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-150x235.png 150w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_.png 200w\" sizes=\"(max-width: 12px) 100vw, 12px\" \/><\/span><\/em><\/a><\/span><\/span><\/h4>\n<p>\u00a0<\/p>\n<h4><span style=\"color: #008000;\"><a href=\"https:\/\/journals.aps.org\/prl\/abstract\/10.1103\/PhysRevLett.122.043903\">Anderson photon-phonon co-localization in certain random superlattices<\/a><br \/><\/span><span style=\"color: #008000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt; color: #000000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\">G. Arregui,\u00a0\u00a0<\/span><\/span><\/span><span style=\"color: #000000; font-family: tahoma, arial, helvetica, sans-serif; font-size: 13.3333px;\">N. D. Lanzillotti-Kimura,\u00a0<\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">C. M. Sotomayor-Torres, P. D. Garc\u00eda<\/span><br \/><\/span><span style=\"color: #000000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt; color: #000000;\"><span style=\"font-size: 10pt;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\">Phys. Rev. Lett.\u00a0<strong>122<\/strong>, 043903, 2019\u00a0<\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><em style=\"color: #008000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><img decoding=\"async\" loading=\"lazy\" class=\"alignnone wp-image-269\" src=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-192x300.png\" alt=\"\" width=\"12\" height=\"19\" srcset=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-192x300.png 192w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-100x157.png 100w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_-150x235.png 150w, http:\/\/nanophononics.eu\/wp-content\/uploads\/2018\/10\/200px-Open_Access_logo_PLoS_white.svg_.png 200w\" sizes=\"(max-width: 12px) 100vw, 12px\" \/><\/span><\/em><\/span><\/span><\/span><\/span><\/h4>\n\n\n\n<div class=\"is-layout-flex wp-container-3 wp-block-columns\">\n<div class=\"is-layout-flow wp-block-column\">\n<h4><a href=\"http:\/\/nanophononics.eu\/?page_id=1385\">2020<\/a><\/h4>\n<\/div>\n\n\n\n<div class=\"is-layout-flow wp-block-column\">\n<h4 class=\"has-text-align-right\"><a href=\"http:\/\/nanophononics.eu\/?page_id=1403\">2018<\/a><\/h4>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>Phonon engineering with superlattices: generalized nanomechanical potentialsO. Ortiz, M. Esmann, N. D. Lanzillotti-KimuraPhys. Rev. B\u00a0100, 085430, 2019 \u00a0 Brillouin scattering in hybrid optophononic Bragg micropillar resonators at 300GHzM. Esmann, F. R. Lamberti, A. Harouri, L. Lanco, I. Sagnes, I. Favero, G. Aubin, C. Gomez-Carbonell, A. Lemaitre, O. Krebs, P. Senellart, N. D. Lanzillotti-KimuraOptica 6, 854,<\/p><\/div>\n<div class=\"blog-btn\"><a href=\"http:\/\/nanophononics.eu\/?page_id=1329\" class=\"home-blog-btn\">Read More<\/a><\/p>\n","protected":false},"author":4,"featured_media":0,"parent":1343,"menu_order":1,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_eb_attr":""},"_links":{"self":[{"href":"http:\/\/nanophononics.eu\/index.php?rest_route=\/wp\/v2\/pages\/1329"}],"collection":[{"href":"http:\/\/nanophononics.eu\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"http:\/\/nanophononics.eu\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"http:\/\/nanophononics.eu\/index.php?rest_route=\/wp\/v2\/users\/4"}],"replies":[{"embeddable":true,"href":"http:\/\/nanophononics.eu\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=1329"}],"version-history":[{"count":12,"href":"http:\/\/nanophononics.eu\/index.php?rest_route=\/wp\/v2\/pages\/1329\/revisions"}],"predecessor-version":[{"id":1426,"href":"http:\/\/nanophononics.eu\/index.php?rest_route=\/wp\/v2\/pages\/1329\/revisions\/1426"}],"up":[{"embeddable":true,"href":"http:\/\/nanophononics.eu\/index.php?rest_route=\/wp\/v2\/pages\/1343"}],"wp:attachment":[{"href":"http:\/\/nanophononics.eu\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=1329"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}