{"id":687,"date":"2015-09-03T08:02:53","date_gmt":"2015-09-02T23:02:53","guid":{"rendered":"https:\/\/enemat.energy.nagoya-u.ac.jp\/?p=687"},"modified":"2021-04-28T08:59:50","modified_gmt":"2021-04-27T23:59:50","slug":"j-appl-phys-%e7%89%b9%e9%9b%86%e5%8f%b7","status":"publish","type":"post","link":"https:\/\/enemat.energy.nagoya-u.ac.jp\/en\/2015\/09\/03\/687\/","title":{"rendered":"Published: Negligible clamping effect in (111)-Pb(Zr,Ti)O3 films"},"content":{"rendered":"\n<p>Our paper entitled &#8220;<em>Negligible substrate clamping effect on piezoelectric response in (111)-epitaxial tetragonal Pb(Zr, Ti)O<sub>3<\/sub>&nbsp;films<\/em>&#8221; has been published in J. Appl. Phys. The 3D-plot of time-resolved synchrotron XRD was incorporated into the cover image (bottom left).<\/p>\n\n\n\n<p>Citation:&nbsp;<a href=\"http:\/\/dx.doi.org\/10.1063\/1.4927810\">J. Appl. Phys.&nbsp;<strong>118<\/strong>, 072012 (2015)<\/a><\/p>\n\n\n\n<figure class=\"wp-block-gallery columns-1 is-cropped wp-block-gallery-1 is-layout-flex wp-block-gallery-is-layout-flex\"><ul class=\"blocks-gallery-grid\"><li class=\"blocks-gallery-item\"><figure><img loading=\"lazy\" decoding=\"async\" width=\"225\" height=\"300\" src=\"https:\/\/enemat.energy.nagoya-u.ac.jp\/wordpress\/wp-content\/uploads\/2021\/04\/jap_cover-225x300.jpg\" alt=\"\" data-id=\"181\" data-full-url=\"https:\/\/enemat.energy.nagoya-u.ac.jp\/wordpress\/wp-content\/uploads\/2021\/04\/jap_cover.jpg\" data-link=\"https:\/\/enemat.energy.nagoya-u.ac.jp\/jap_cover\/\" class=\"wp-image-181\" srcset=\"https:\/\/enemat.energy.nagoya-u.ac.jp\/wordpress\/wp-content\/uploads\/2021\/04\/jap_cover-225x300.jpg 225w, https:\/\/enemat.energy.nagoya-u.ac.jp\/wordpress\/wp-content\/uploads\/2021\/04\/jap_cover.jpg 371w\" sizes=\"auto, (max-width: 225px) 100vw, 225px\" \/><\/figure><\/li><\/ul><\/figure>\n","protected":false},"excerpt":{"rendered":"<p>Our paper entitled &#8220;Negligible substrate clamping effect on piezoelectric response in (111)-epitaxial tetragonal Pb(Zr, Ti)O3&nbsp;films&#8221; has been published in J. Appl. Phys. The 3D-plot of time-resolved synchrotron XRD was incorporated into the cover image (bottom left). Citation:&nbsp;J. Appl. Phys.&nbsp;118, 072012 (2015)<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_locale":"en_US","_original_post":"https:\/\/enemat.energy.nagoya-u.ac.jp\/?p=339","footnotes":""},"categories":[1],"tags":[],"class_list":["post-687","post","type-post","status-publish","format-standard","hentry","category-uncategorized","en-US"],"_links":{"self":[{"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/posts\/687","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/comments?post=687"}],"version-history":[{"count":1,"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/posts\/687\/revisions"}],"predecessor-version":[{"id":688,"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/posts\/687\/revisions\/688"}],"wp:attachment":[{"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/media?parent=687"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/categories?post=687"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/enemat.energy.nagoya-u.ac.jp\/wp-json\/wp\/v2\/tags?post=687"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}