{"id":1363,"date":"2017-05-08T14:00:42","date_gmt":"2017-05-08T13:00:42","guid":{"rendered":"http:\/\/www.icmm.csic.es\/eosmad\/?page_id=1363"},"modified":"2017-05-08T14:00:42","modified_gmt":"2017-05-08T13:00:42","slug":"magnetoelectric-characterization-lab","status":"publish","type":"page","link":"https:\/\/wp.icmm.csic.es\/eosmad\/labs-techs\/magnetoelectric-characterization-lab\/","title":{"rendered":"magnetoelectric characterization Lab"},"content":{"rendered":"<h4>(contact person: <a href=\"mailto:malguero@icmm.csic.es\">Dr. Miguel Alguer\u00f3<\/a>)<\/h4>\n<h4><a href=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-characterization-equipment.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-1365 size-full alignnone\" src=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-characterization-equipment.jpg\" alt=\"Magnetoelectric characterization equipment\" width=\"904\" height=\"457\" srcset=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-characterization-equipment.jpg 904w, https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-characterization-equipment-300x152.jpg 300w, https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-characterization-equipment-768x388.jpg 768w, https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-characterization-equipment-750x380.jpg 750w\" sizes=\"auto, (max-width: 904px) 100vw, 904px\" \/><\/a><a href=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-measurement.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-1368 alignleft\" src=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-measurement-300x267.jpg\" alt=\"Magnetoelectric measurement\" width=\"300\" height=\"267\" srcset=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-measurement-300x267.jpg 300w, https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-measurement.jpg 328w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/h4>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>Magnetoelectric measurements are carried out using an experimental setup that contains a combination of two Helmholtz coils: a high power coil and a high frequency one, designed to independently provide a static increasingly high magnetic field up to 1 kOe (magnetization field), and an alternate magnetic field of 10 Oe at varying frequencies between 1 kHz and 200 kHz (the stimulus), respectively. The output voltages developed as a response of the alternate magnetic field are monitored with a lock-in amplifier.<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>Examples of measurements carried out with this equipment can be found in the following publications:<\/p>\n<p><a href=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-Nature-Comm.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-1378 alignleft\" src=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-Nature-Comm-300x234.jpg\" alt=\"Magnetoelectric curve Nature Comm\" width=\"300\" height=\"234\" srcset=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-Nature-Comm-300x234.jpg 300w, https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-Nature-Comm.jpg 594w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n<p>&nbsp;<\/p>\n<p><b><a href=\"http:\/\/www.nature.com\/articles\/ncomms12772\" target=\"_blank\">A novel perovskite oxide chemically designed to show multiferroic phase boundary with room-temperature magnetoelectricity<\/a><\/b><br \/>\nFern\u00e1ndez-Posada, CM; Castro, A; Kiat, J-M; Porcher, F; Pe\u00f1a, O; Alguer\u00f3, M; Amor\u00edn, H<br \/>\n<span style=\"color: #993300\"><strong>Nature Communications<\/strong><\/span> 7, 12772 (2016)<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><a href=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-Mater-Design.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-1379 alignleft\" src=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-Mater-Design-300x229.jpg\" alt=\"Magnetoelectric curve Mater Design\" width=\"300\" height=\"229\" srcset=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-Mater-Design-300x229.jpg 300w, https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-Mater-Design.jpg 545w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n<p>&nbsp;<\/p>\n<p><strong><a href=\"http:\/\/www.sciencedirect.com\/science\/article\/pii\/S0264127516309066\" target=\"_blank\">Point defect engineering of high temperature piezoelectric BiScO3-PbTiO3 for enhanced voltage response<\/a><\/strong><b><\/b><br \/>\nPascual-Gonz\u00e1lez, C; Berganza, E; Amor\u00edn, H; Castro, A; Alguer\u00f3, M<br \/>\n<span style=\"color: #c0504d\"><strong>Materials &amp; Design<\/strong><\/span> 108, 501\u2013509 (2016)<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><a href=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-JACERS.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-1380 alignleft\" src=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-JACERS-300x232.jpg\" alt=\"Magnetoelectric curve JACERS\" width=\"300\" height=\"232\" srcset=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-JACERS-300x232.jpg 300w, https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-JACERS.jpg 571w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n<p>&nbsp;<\/p>\n<p><b><a href=\"http:\/\/onlinelibrary.wiley.com\/doi\/10.1111\/jace.14131\/full\" target=\"_blank\">Yttrium iron garnet\/barium titanate multiferroic composites<\/a><\/b><br \/>\nSchileo, G; Pascual-Gonz\u00e1lez, C; Alguer\u00f3, M; Reaney, IM; Postolache, P; Mitoseriu, L; Reichmann, K; Feteira, A<br \/>\n<span style=\"color: #c0504d\"><strong>Journal of the American\u00a0Ceramic Society<\/strong><\/span> 99, 1609-1614 (2016)<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><a href=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-STAM.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-1381 alignleft\" src=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-STAM-192x300.jpg\" alt=\"Magnetoelectric curve STAM\" width=\"286\" height=\"447\" srcset=\"https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-STAM-192x300.jpg 192w, https:\/\/wp.icmm.csic.es\/eosmad\/wp-content\/uploads\/sites\/31\/2017\/05\/Magnetoelectric-curve-STAM.jpg 509w\" sizes=\"auto, (max-width: 286px) 100vw, 286px\" \/><\/a><\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><b><a href=\"http:\/\/iopscience.iop.org\/article\/10.1088\/1468-6996\/16\/1\/016001\" target=\"_blank\">High-sensitivity piezoelectric perovskites for magnetoelectric composites<\/a><\/b><br \/>\nAmor\u00edn, H; Alguer\u00f3, M; Del Campo, R; Vila, E; Ramos, P; Doll\u00e9, M; Romaguera-Barcelay, Y; De La Cruz, JP; Castro, A<br \/>\n<span style=\"color: #c0504d\"><strong>Science and Technology of Advanced Materials<\/strong><\/span> 16, 016001 (2015)<\/p>\n","protected":false},"excerpt":{"rendered":"<p>(contact person: Dr. Miguel Alguer\u00f3) &nbsp; &nbsp; Magnetoelectric measurements are carried out using an experimental setup that contains a combination of two Helmholtz coils: a&#8230;<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":13,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"page-template-fullwidth.php","meta":{"ngg_post_thumbnail":0,"footnotes":""},"class_list":["post-1363","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/wp.icmm.csic.es\/eosmad\/wp-json\/wp\/v2\/pages\/1363","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/wp.icmm.csic.es\/eosmad\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/wp.icmm.csic.es\/eosmad\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/wp.icmm.csic.es\/eosmad\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/wp.icmm.csic.es\/eosmad\/wp-json\/wp\/v2\/comments?post=1363"}],"version-history":[{"count":0,"href":"https:\/\/wp.icmm.csic.es\/eosmad\/wp-json\/wp\/v2\/pages\/1363\/revisions"}],"up":[{"embeddable":true,"href":"https:\/\/wp.icmm.csic.es\/eosmad\/wp-json\/wp\/v2\/pages\/13"}],"wp:attachment":[{"href":"https:\/\/wp.icmm.csic.es\/eosmad\/wp-json\/wp\/v2\/media?parent=1363"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}