{"id":2572,"date":"2021-10-01T07:26:09","date_gmt":"2021-10-01T07:26:09","guid":{"rendered":"https:\/\/www.polimix.fisi.polimi.it\/?p=2572"},"modified":"2021-10-01T07:43:28","modified_gmt":"2021-10-01T07:43:28","slug":"restored-strange-metal-phase-through-suppression-ofcharge-density-waves-in-underdoped-yba2cu3o7-d","status":"publish","type":"post","link":"https:\/\/www.polimix.fisi.polimi.it\/?p=2572","title":{"rendered":"Restored strange metal phase through suppression of charge density waves in underdoped YBa2Cu3O7-\u03b4"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-post\" data-elementor-id=\"2572\" class=\"elementor elementor-2572\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-7a7c6e7f elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"7a7c6e7f\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-3ad40e04\" data-id=\"3ad40e04\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-inner-section elementor-element elementor-element-e21cfbe elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"e21cfbe\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-inner-column elementor-element elementor-element-88ad35b\" data-id=\"88ad35b\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-9d57763 elementor-widget elementor-widget-text-editor\" data-id=\"9d57763\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><a href=\"https:\/\/www.science.org\/doi\/10.1126\/science.abc8372\">Restored strange metal phase through suppression of&nbsp;charge density waves in underdoped YBa<sub>2<\/sub>Cu<sub>3<\/sub>O<sub>7-\u03b4<\/sub><\/a><\/p>\n<p>The normal state of optimally doped cuprates is dominated by the \u201cstrange metal\u201d phase that shows a linear temperature (T) dependence of the resistivity persisting down to the lowest T. For underdoped cuprates, this behavior is lost below the pseudogap temperature T*, where charge density waves (CDWs), together with other intertwined local orders, characterize the ground state. We found that the T-linear resistivity of highly strained, ultrathin, underdoped YBa2Cu3O7\u2013d films is restored when the CDW amplitude, detected by resonant inelastic x-ray scattering, is suppressed. This observation suggests an intimate connection between the onset of CDWs and the departure from T-linear resistivity in underdoped cuprates. Our results illustrate the potential of using strain control to manipulate the ground state of quantum materials.<\/p><p><br><\/p>\n<p>Science, 373 (6562)<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-inner-column elementor-element elementor-element-0a9c2cc\" data-id=\"0a9c2cc\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-3876895 elementor-widget elementor-widget-image\" data-id=\"3876895\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img fetchpriority=\"high\" decoding=\"async\" width=\"569\" height=\"569\" src=\"https:\/\/www.polimix.fisi.polimi.it\/wp-content\/uploads\/2021\/10\/Science.png\" class=\"attachment-large size-large wp-image-2573\" alt=\"\" srcset=\"https:\/\/www.polimix.fisi.polimi.it\/wp-content\/uploads\/2021\/10\/Science.png 569w, https:\/\/www.polimix.fisi.polimi.it\/wp-content\/uploads\/2021\/10\/Science-300x300.png 300w, https:\/\/www.polimix.fisi.polimi.it\/wp-content\/uploads\/2021\/10\/Science-150x150.png 150w, https:\/\/www.polimix.fisi.polimi.it\/wp-content\/uploads\/2021\/10\/Science-450x450.png 450w\" sizes=\"(max-width: 569px) 100vw, 569px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>Restored strange metal phase through suppression of&nbsp;charge density waves in underdoped YBa2Cu3O7-\u03b4 The normal state of optimally doped cuprates is dominated by the \u201cstrange metal\u201d phase that shows a linear temperature (T) dependence of the resistivity persisting down to the lowest T. For underdoped cuprates, this behavior is lost below the pseudogap temperature T*, where [&hellip;]<\/p>\n","protected":false},"author":8,"featured_media":2573,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[7],"tags":[],"class_list":["post-2572","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-publications"],"_links":{"self":[{"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=\/wp\/v2\/posts\/2572","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=\/wp\/v2\/users\/8"}],"replies":[{"embeddable":true,"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=2572"}],"version-history":[{"count":15,"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=\/wp\/v2\/posts\/2572\/revisions"}],"predecessor-version":[{"id":2590,"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=\/wp\/v2\/posts\/2572\/revisions\/2590"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=\/wp\/v2\/media\/2573"}],"wp:attachment":[{"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=2572"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=2572"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.polimix.fisi.polimi.it\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=2572"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}