{"id":1362,"date":"2024-08-29T15:39:00","date_gmt":"2024-08-29T13:39:00","guid":{"rendered":"http:\/\/nanophononics.eu\/?page_id=1362"},"modified":"2025-01-13T15:02:03","modified_gmt":"2025-01-13T14:02:03","slug":"2023-2","status":"publish","type":"page","link":"http:\/\/nanophononics.eu\/?page_id=1362","title":{"rendered":"2023"},"content":{"rendered":"\n\n\n<h4><a href=\"https:\/\/opg.optica.org\/ome\/fulltext.cfm?uri=ome-13-12-3715&amp;id=543988\">Design of cost-effective environment-responsive nanoacoustic devices based on mesoporous thin films<\/a><br \/><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">Edson R. Cardozo de Oliveira, Priscila Vensaus, Galo J. A. A. Soler-Illia, and Norberto Daniel Lanzillotti-Kimura<br \/>Opt. Mater. Express <b>13<\/b>, 3715-3726 (2023) <\/span><\/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=\"wp-image-269 alignnone\" 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:\/\/link.aps.org\/doi\/10.1103\/PhysRevB.108.205301\">Topological nanophononic interface states using high-order bandgaps in the one-dimensional Su-Schrieffer-Heeger model<\/a><br \/><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">A. Rodriguez, K. Papatryfonos, E. Cardozo de Oliveira, N. D. Lanzillotti-Kimura<br \/>Phys. Rev. B 108, 205301, 2023 <\/span><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\"><em style=\"color: #008000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><img decoding=\"async\" loading=\"lazy\" class=\"wp-image-269 alignnone\" 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<h4>\u00a0<\/h4>\n<h4><span style=\"color: #008000;\"><a href=\"https:\/\/pubs.acs.org\/doi\/abs\/10.1021\/acsphotonics.3c00186\">Brillouin Scattering Selection Rules in Polarization-Sensitive Photonic Resonators<\/a><br \/><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">A. Rodriguez, P. Priya, E. Cardozo de Oliveira, L. Le Gratiet, I. Sagnes, M. Morassi, A. Lema\u00eetre, F. Pastier, L. Lanco, M. Esmann, N. D. Lanzillotti-Kimura<br \/><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><span style=\"font-size: 13.3333px;\">ACS Photonics <strong>10<\/strong>, 1687, 2023<\/span><\/span> <\/span><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\"><em style=\"color: #008000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><img decoding=\"async\" loading=\"lazy\" class=\"wp-image-269 alignnone\" 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=\"color: #008000;\"><a href=\"https:\/\/doi.org\/10.1016\/j.optlastec.2023.109130\">Genetic optimization of Brillouin scattering gain in subwavelength-structured silicon membrane waveguides<\/a><br \/><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">P. Nu\u00f1o Ruano, J. Zhang, D. Melati, D. Gonz\u00e1lez-Andrade, X. Le Roux, E. Cassan, D. Marris-Morini, L. Vivien, N. D. Lanzillotti-Kimura, C. Alonso-Ramos<br \/>Optics &amp; Laser Technology 161, 109130, 2023 <\/span><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\"><em style=\"color: #008000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><img decoding=\"async\" loading=\"lazy\" class=\"wp-image-269 alignnone\" 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=\"color: #008000;\"><a href=\"https:\/\/doi.org\/10.1515\/nanoph-2022-0780\">Towards chiral acoustoplasmonics<\/a><br \/><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">B. Castillo Lopez de Larrinzar, C. Xiang, E. Cardozo de Oliveira, N. D. Lanzillotti-Kimura, A. Garcia Martin<br \/>Nanophotonics 12, 1957, 2023 <\/span><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\"><em style=\"color: #008000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><img decoding=\"async\" loading=\"lazy\" class=\"wp-image-269 alignnone\" 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<p><span style=\"font-family: tahoma, arial, helvetica, sans-serif; color: #008000; font-size: 10pt;\"><img decoding=\"async\" loading=\"lazy\" class=\"wp-image-873 alignright\" src=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/apl.2023.122.issue-14.largecover-223x300.jpg\" alt=\"\" width=\"200\" height=\"270\" srcset=\"http:\/\/nanophononics.eu\/wp-content\/uploads\/apl.2023.122.issue-14.largecover-223x300.jpg 223w, http:\/\/nanophononics.eu\/wp-content\/uploads\/apl.2023.122.issue-14.largecover-1144x1536.jpg 1144w\" sizes=\"(max-width: 200px) 100vw, 200px\" \/><\/span><\/p>\n<h4><span style=\"color: #008000;\"><a href=\"https:\/\/doi.org\/10.1063\/5.0142925\">Perspectives on high-frequency nanomechanics, nanoacoustics and nanophononics<\/a><br \/><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">Priya, E. R. Cardozo de Oliveira, N. D. Lanzillotti-Kimura<br \/>Appl. Phys. Lett. 122, 140501, 2023 <\/span><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\"><em style=\"color: #008000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><img decoding=\"async\" loading=\"lazy\" class=\"wp-image-269 alignnone\" 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=\"color: #008000;\"><a href=\"https:\/\/doi.org\/10.1016\/j.pacs.2023.100472\">Probing Gigahertz Coherent Acoustic Phonons in TiO2 Mesoporous Thin Films<\/a><br \/><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\">E. R. Cardozo de Oliveira, C. Xiang, M. Esmann, N. Lopez Abdala, M. C. Fuertes, A. Bruchhausen, H. Pastoriza, B. Perrin, G. J. A. A. Soler-Illia, N. D. Lanzillotti-Kimura<br \/>Photoacoustics 30, 100472, 2023 <\/span><\/span><span style=\"font-family: tahoma, arial, helvetica, sans-serif; font-size: 10pt;\"><span style=\"color: #000000;\"><em style=\"color: #008000;\"><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><img decoding=\"async\" loading=\"lazy\" class=\"wp-image-269 alignnone\" 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><br \/><br \/><span style=\"font-family: tahoma, arial, helvetica, sans-serif;\"><span style=\"font-size: 13.3333px;\">\u00a0<\/span><\/span><\/p>\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=1379\">2024<\/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=1371\">2022<\/a><\/h4>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>Design of cost-effective environment-responsive nanoacoustic devices based on mesoporous thin filmsEdson R. Cardozo de Oliveira, Priscila Vensaus, Galo J. A. A. Soler-Illia, and Norberto Daniel Lanzillotti-KimuraOpt. Mater. Express 13, 3715-3726 (2023) \u00a0 Topological nanophononic interface states using high-order bandgaps in the one-dimensional Su-Schrieffer-Heeger modelA. Rodriguez, K. Papatryfonos, E. Cardozo de Oliveira, N. D. Lanzillotti-KimuraPhys. Rev.<\/p><\/div>\n<div class=\"blog-btn\"><a href=\"http:\/\/nanophononics.eu\/?page_id=1362\" 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\/1362"}],"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=1362"}],"version-history":[{"count":9,"href":"http:\/\/nanophononics.eu\/index.php?rest_route=\/wp\/v2\/pages\/1362\/revisions"}],"predecessor-version":[{"id":1609,"href":"http:\/\/nanophononics.eu\/index.php?rest_route=\/wp\/v2\/pages\/1362\/revisions\/1609"}],"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=1362"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}