{"id":23009,"date":"2024-08-01T14:38:39","date_gmt":"2024-08-01T17:38:39","guid":{"rendered":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/?p=23009"},"modified":"2024-08-01T14:38:40","modified_gmt":"2024-08-01T17:38:40","slug":"new-development-of-skutterudite-type-thermoelectric-materials-using-high-pressure-technique-com-prof-chihiro-sekine","status":"publish","type":"post","link":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/new-development-of-skutterudite-type-thermoelectric-materials-using-high-pressure-technique-com-prof-chihiro-sekine\/","title":{"rendered":"New development of skutterudite-type thermoelectric materials using high-pressure technique, com Prof. Chihiro Sekine"},"content":{"rendered":"\n<p>Partially filled skutterudite compounds have been considered as potential candidates for highly efficient thermoelectric materials. The unfilled skutterudite compound MX3 (M = Co, Rh and Ir, X = P, As and Sb), which is a cage-like material, shows excellent thermoelectric (TE) performance. However, the compounds have a disadvantage of high lattice thermal conductivity \u03baL compared to conventional TE materials. The vacancy inside the cage of MX3 (M4X12) can accept a relatively small guest ion R. The vacancy can be partially occupied by R (RxM4X12), such as alkaline-earth, rare-earth and group 13 elements, resulting in a large decrease in \u03baL and improve the TE performance. Namely, R ions are located inside the cages and a marked rattling effect occurs. The reduction in \u03baL for a partially filled skutterudite is a promising method for improving the TE performance. For several RxM4X12, \u03baL decreases with increasing filling ratio x of guest ions. Therefore, partially filled skutterudite compounds with high filling ratio are expected for high-performance TE materials. High pressure benefits the entrance of R into the voids of unfilled skutterudite structure than ambient pressure. We have succeeded in filling unfilled skutterudite compounds with R at a high filling rate x by high-pressure synthesis. Furthermore, we succeeded in filling heavy rare earth ions (Tb and Dy), which cannot be filled at ambient pressure. In this study, we also focused on a pressure-induced self-insertion reaction. Namely, X atom enters the void of X cage by the reaction under high pressure. The \u03baL of SbxM4Sb12-x (M = Co and Rh) were significantly reduced. This suggests that the pressure-induced structural change could be beneficial for improving TE performance.<\/p>\n\n\n\n<p>Prof. Sekine is a Visiting Researcher at LQMEC hosted by Prof. Larrea inside the PRINT USP CAPES grant.<\/p>\n\n\n\n<p><em>New development of skutterudite-type thermoelectric materials using high-pressure technique<br>LQMEC Synergy com Prof. Chihiro Sekine (Muroran Institute of Technology)<br>21\/08, 4\u00aa feira, 15h. No Instituto de F\u00edsica da USP &#8211; Ed. Principal, audit\u00f3rio Marcello Damy. Via Zoom: sala 894 3319 0915 senha 469640 (<a href=\"https:\/\/usp-br.zoom.us\/j\/89433190915\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/usp-br.zoom.us\/j\/89433190915<\/a>)<\/em><\/p>\n\n\n\n<p>*Informa\u00e7\u00f5es dispon\u00edveis em&nbsp;<a href=\"https:\/\/portal.if.usp.br\/ifusp\/pt-br\/evento\/new-development-skutterudite-type-thermoelectric-materials-using-high-pressure-technique\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/portal.if.usp.br\/ifusp\/pt-br\/evento\/new-development-skutterudite-type-thermoelectric-materials-using-high-pressure-technique<\/a><\/p>\n\n\n\n<p><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Partially filled skutterudite compounds have been considered as potential candidates for highly efficient thermoelectric materials. The unfilled skutterudite compound MX3 (M = Co, Rh and Ir, X = P, As and Sb), which is a cage-like material, shows excellent thermoelectric (TE) performance. However, the compounds have a disadvantage of high lattice thermal conductivity \u03baL compared [&hellip;]<\/p>\n","protected":false},"author":4,"featured_media":16567,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[461],"tags":[],"class_list":["post-23009","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-eventos"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/posts\/23009","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/users\/4"}],"replies":[{"embeddable":true,"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/comments?post=23009"}],"version-history":[{"count":1,"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/posts\/23009\/revisions"}],"predecessor-version":[{"id":23010,"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/posts\/23009\/revisions\/23010"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/media\/16567"}],"wp:attachment":[{"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/media?parent=23009"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/categories?post=23009"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.sbfisica.org.br\/v1\/sbf\/wp-json\/wp\/v2\/tags?post=23009"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}