{"id":791,"date":"2022-12-16T10:03:37","date_gmt":"2022-12-16T09:03:37","guid":{"rendered":"https:\/\/ultimate-i.eu\/?p=791"},"modified":"2022-12-18T11:05:56","modified_gmt":"2022-12-18T10:05:56","slug":"a-seminar-entitled-strain-effects-in-vanadium-dioxide-films-with-metal-insulator-electronic-transition","status":"publish","type":"post","link":"https:\/\/ultimate-i.eu\/index.php\/2022\/12\/16\/a-seminar-entitled-strain-effects-in-vanadium-dioxide-films-with-metal-insulator-electronic-transition\/","title":{"rendered":"A seminar entitled &#8220;Strain effects in vanadium dioxide films with metal-insulator electronic transition&#8221;"},"content":{"rendered":"\n<p>Friday, December 16, at 11 a.m. Buenos Aires Time,  Prof. Dr Jos\u00e9 Santiso gave a seminar entitled &#8220;Strain effects in vanadium dioxide films with the metal-insulator electronic transition&#8221; at <a href=\"http:\/\/ultimate-i.eu\/index.php\/consejo-nacional-de-investigaciones-cientificas-y-tecnicas\/\"><strong>&#8220;Laboratorio de F\u00edsica de Superficies e Interfaces&#8221;, Instituto de F\u00edsica del Litoral (IFIS-Litoral, CONICET-UNL)<\/strong>. <\/a><br><br>Jos\u00e9 Santiso is a researcher at the <a href=\"http:\/\/ultimate-i.eu\/index.php\/institut-catala-de-nanociencia-i-nanotecnologia\/\">Catalan Institute of Nanoscience and Nanotechnology (ICN2)<\/a> in Barcelona, Spain. Dr Santiso, invited by Dr Mario C. G. Passeggih is part of the ULTIMATE-I (Ultra Thin Magneto Thermal Sensoring) project supported by the European Union.<\/p>\n\n\n\n<figure class=\"wp-block-gallery has-nested-images columns-default is-cropped wp-block-gallery-1 is-layout-flex wp-block-gallery-is-layout-flex\">\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1599\" height=\"1200\" data-id=\"797\" src=\"http:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.56.49.jpg\" alt=\"\" class=\"wp-image-797\" srcset=\"https:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.56.49.jpg 1599w, https:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.56.49-300x225.jpg 300w, https:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.56.49-1024x768.jpg 1024w, https:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.56.49-768x576.jpg 768w, https:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.56.49-1536x1153.jpg 1536w\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" \/><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1200\" height=\"1599\" data-id=\"798\" src=\"http:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.57.21.jpg\" alt=\"\" class=\"wp-image-798\" srcset=\"https:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.57.21.jpg 1200w, https:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.57.21-225x300.jpg 225w, https:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.57.21-768x1023.jpg 768w, https:\/\/ultimate-i.eu\/wp-content\/uploads\/2022\/12\/WhatsApp-slika-2022-12-16-u-19.57.21-1153x1536.jpg 1153w\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" \/><\/figure>\n<\/figure>\n\n\n\n<p>The following is a brief summary.<\/p>\n\n\n\n<p>Vanadium dioxide (VO<sub>2<\/sub>)is an archetypical material showing a metal-insulator (M-I) Mott transition at&nbsp;about T=68C with several orders of magnitude change in the resistivity between the&nbsp;semiconducting low-T M1 phase and the high-T metallic rutile R phase. It has been proposed as a&nbsp;good candidate directly for Resistive-Random Access Memory (RRAM) devices or as complementary&nbsp;selector in combination of a bipolar RRAM device because of its high on\/off ratio, fast switching&nbsp;speed and high current density. Although in bulk form the transition is above room temperature&nbsp;either chemical doping or mechanical strain have been demonstrated to bring the transition closer&nbsp;or even below room temperature making it very attractive in different devices. This work studies the&nbsp;structure features across transition of high quality strained epitaxial VO<sub>2<\/sub> films deposited on&nbsp;isostructural rutile TiO<sub>2<\/sub> (001) single crystals. Since M-I transition in VO<sub>2<\/sub> is accompanied by a structural&nbsp;change between monoclinic M1 phase and tetragonal R phase, with substantial variation in cell&nbsp;parameters, the nucleation of the high-T R phase embedded in the low-T M1 phase during&nbsp;transition, is expected to generate local interfacial regions with a large strain. The characterization of&nbsp;the structural features of the films by means of synchrotron X-ray Diffraction upon thermal cycles&nbsp;revealed the formation of local strain effects during the phase transition in competition with the&nbsp;epitaxial strain induced by the growth on the mismatched TiO<sub>2<\/sub> substrates. Such interphase regions&nbsp;between M1 and R crystal domains are submitted to a uniaxial strain (overlapped to the biaxial in-plane epitaxial strain) that stabilizes other polytypic VO<sub>2<\/sub> insulating phases (monoclinic M2, and&nbsp;triclinic transitional M3 or T phase) beyond their expected stability regions.[1] Concomitant to the subtle structural distortions a slight rotation of the monoclinic crystal domains occurs to&nbsp;accommodate the elastic energy constraints. The persistence of the coexistence of those polytypic&nbsp;phases even at room temperature turns VO<sub>2<\/sub> into a complex heterogeneous material. Nonetheless, at&nbsp;conditions where XRD of the films seems to indicate a pure rutile R phase, HRTEM analysis revealed&nbsp;a certain degree of heterogeneity at the nanoscale forming an intricate tweed pattern of other&nbsp;polytypes with different arrangements of V-V dimers along the c-axis direction [2], still displaying a&nbsp;metallic character. Altogether these observations evidence that VO<sub>2<\/sub> micro and nanostructure, and&nbsp;therefore its electrical response, depends on a subtle balance of unconventional strain relaxation&nbsp;mechanisms.<\/p>\n\n\n\n<p>[1] L. Rodr\u00edguez, F. Sandiumenge, C. Frontera, J.M. Caicedo, J. Padilla, G. Catal\u00e1n, J. Santiso, Strong&nbsp;strain gradients and phase coexistence at the metal-insulator transition in VO<sub>2<\/sub> epitaxial films, Acta&nbsp;Mater. 220 (2021) 117336.<\/p>\n\n\n\n<p>[2] F. Sandiumenge, L. Rodr\u00edguez, M. Pruneda, C. Mag\u00e9n, J. Santiso, G. Catalan, Metallic Diluted&nbsp;Dimerization in VO<sub>2<\/sub> Tweeds, Adv. Mater. 33 (2021) 2004374.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Friday, December 16, at 11 a.m. Buenos Aires Time, Prof. Dr Jos\u00e9 Santiso gave a seminar entitled &#8220;Strain effects in vanadium dioxide films with the metal-insulator electronic transition&#8221; at &#8220;Laboratorio de F\u00edsica de Superficies e Interfaces&#8221;, Instituto de F\u00edsica del Litoral (IFIS-Litoral, CONICET-UNL). Jos\u00e9 Santiso is a researcher at the Catalan Institute of Nanoscience and &hellip; <\/p>\n<p class=\"link-more\"><a href=\"https:\/\/ultimate-i.eu\/index.php\/2022\/12\/16\/a-seminar-entitled-strain-effects-in-vanadium-dioxide-films-with-metal-insulator-electronic-transition\/\" class=\"more-link\">Continue reading<span class=\"screen-reader-text\"> &#8220;A seminar entitled &#8220;Strain effects in vanadium dioxide films with metal-insulator electronic transition&#8221;&#8221;<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"categories":[1],"tags":[],"post_formats":[],"class_list":["post-791","post","type-post","status-publish","format-standard","hentry","category-non-classe"],"aioseo_notices":[],"guten_post_layout_featured_media_urls":{"full":false,"thumbnail":false,"medium":false,"medium_large":false,"large":false,"1536x1536":false,"2048x2048":false,"guten_post_layout_landscape_large":false,"guten_post_layout_portrait_large":false,"guten_post_layout_square_large":false,"guten_post_layout_landscape":false,"guten_post_layout_portrait":false,"guten_post_layout_square":false,"twentyseventeen-featured-image":false,"twentyseventeen-thumbnail-avatar":false},"_links":{"self":[{"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/posts\/791","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/comments?post=791"}],"version-history":[{"count":3,"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/posts\/791\/revisions"}],"predecessor-version":[{"id":799,"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/posts\/791\/revisions\/799"}],"wp:attachment":[{"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/media?parent=791"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/categories?post=791"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/tags?post=791"},{"taxonomy":"post_format","embeddable":true,"href":"https:\/\/ultimate-i.eu\/index.php\/wp-json\/wp\/v2\/post_formats?post=791"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}