{"id":27336,"date":"2024-06-21T15:36:57","date_gmt":"2024-06-21T07:36:57","guid":{"rendered":"\/phys\/?page_id=27336"},"modified":"2024-06-27T14:41:00","modified_gmt":"2024-06-27T06:41:00","slug":"study-of-the-b-site-substitution-effect-in-the-double-layered-perovskite-ybacufeo%e2%82%85","status":"publish","type":"page","link":"\/phys\/?page_id=27336","title":{"rendered":"Study of the B-site Substitution Effect in the Double-layered Perovskite YBaCuFeO\u2085"},"content":{"rendered":"\n<p class=\"has-medium-font-size\">\u59d3\u540d\uff1a\u5289\u91c7\u9748\uff0c\u6307\u5c0e\u6559\u6388\uff1a\u675c\u662d\u5b8f<\/p>\n\n\n\n<div class=\"wp-block-tkuwpbs5-bs5-container container\" style=\"position:relative\" block_id=\"lxobnzmlee7hkybzqi5\"><style><\/style>\n<div class=\"wp-block-tkuwpbs5-bs5-row row\">\n<div class=\"wp-block-tkuwpbs5-bs5-column col-md-6 align-self-start\">\n<div class=\"wp-block-stackable-image stk-block-image stk-block stk-99e0761\" data-block-id=\"99e0761\"><figure><span class=\"stk-img-wrapper stk-image--shape-stretch\"><img decoding=\"async\" loading=\"lazy\" class=\"stk-img wp-image-27500\" src=\"\/phys\/wp-content\/uploads\/2024\/06\/2024\u6de1\u6c5f\u7269\u7406\u6d77\u5831_\u5289\u91c7\u9748-scaled.jpg\" width=\"1811\" height=\"2560\" srcset=\"\/phys\/wp-content\/uploads\/2024\/06\/2024\u6de1\u6c5f\u7269\u7406\u6d77\u5831_\u5289\u91c7\u9748-scaled.jpg 1811w, \/phys\/wp-content\/uploads\/2024\/06\/2024\u6de1\u6c5f\u7269\u7406\u6d77\u5831_\u5289\u91c7\u9748-212x300.jpg 212w, \/phys\/wp-content\/uploads\/2024\/06\/2024\u6de1\u6c5f\u7269\u7406\u6d77\u5831_\u5289\u91c7\u9748-724x1024.jpg 724w, \/phys\/wp-content\/uploads\/2024\/06\/2024\u6de1\u6c5f\u7269\u7406\u6d77\u5831_\u5289\u91c7\u9748-768x1086.jpg 768w, \/phys\/wp-content\/uploads\/2024\/06\/2024\u6de1\u6c5f\u7269\u7406\u6d77\u5831_\u5289\u91c7\u9748-1086x1536.jpg 1086w, \/phys\/wp-content\/uploads\/2024\/06\/2024\u6de1\u6c5f\u7269\u7406\u6d77\u5831_\u5289\u91c7\u9748-1449x2048.jpg 1449w\" sizes=\"(max-width: 1811px) 100vw, 1811px\" \/><\/span><\/figure><\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-tkuwpbs5-bs5-column col-md-6 align-self-start\">\n<p><strong>Abstract<\/strong><\/p>\n\n\n\n<p>        The double-layered perovskite YBaCuFeO\u2085 (AA\u2019BB\u2019O5) consists of two sublattices of Fe-O and Cu-O aligning alternatively along <em>c<\/em>-axis, and atoms of Y and Ba sit in between sublattices. The YBaCuFeO\u2085 shows a complex magnetic phase diagram, which is mainly due to the coupling between both sublattices. This project aims to understand the magnetic phase transitions by doping different atom to affect the coupling between Fe-O and Cu-O. For doing so, attempt was made to replace Cu<sup>2+<\/sup> with Ni<sup>2+<\/sup>. We have successfully synthesized a series of powder samples of YBaCu1-<em>x<\/em>Ni<em>x<\/em>FeO5 (<em>x <\/em>= 0 ~ 0.7). These powder samples have been refined to have a tetragonal phase with the space group of <em>P<\/em>4\/<em>mmm<\/em>. We confirm the magnetic property of <em>x <\/em>= 0.1 that have antiferromagnetic phase transition of commensurate (CM) to incommensurate (ICM)&nbsp; around the <em>TN<\/em>2 ~ 278K .<\/p>\n<\/div>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>\u59d3\u540d\uff1a\u5289\u91c7\u9748\uff0c\u6307\u5c0e\u6559\u6388\uff1a\u675c\u662d\u5b8f<\/p>\n","protected":false},"author":10,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"wp-custom-template-detail-4-post","meta":{"_uag_custom_page_level_css":"","footnotes":""},"acf":[],"featured_image_urls":{"full":"","thumbnail":"","medium":"","medium_large":"","large":"","twp-icon":"","1536x1536":"","2048x2048":""},"post_excerpt_stackable":"<p>\u59d3\u540d\uff1a\u5289\u91c7\u9748\uff0c\u6307\u5c0e\u6559\u6388\uff1a\u675c\u662d\u5b8f Abstract The double-layered perovskite YBaCuFeO\u2085 (AA\u2019BB\u2019O5) consists of two sublattices of Fe-O and Cu-O aligning alternatively along c-axis, and atoms of Y and Ba sit in between sublattices. The YBaCuFeO\u2085 shows a complex magnetic phase diagram, which is mainly due to the coupling between both sublattices. This project aims to understand the magnetic phase transitions by doping different atom to affect the coupling between Fe-O and Cu-O. For doing so, attempt was made to replace Cu2+ with Ni2+. We have successfully synthesized a series of powder samples of YBaCu1-xNixFeO5 (x = 0 ~ 0.7). These powder samples have been&hellip;<\/p>\n","category_list":"","author_info":{"name":"\u9ec3\u9806\u8208","url":"\/phys\/?author=10"},"comments_num":"0 comments","uagb_featured_image_src":{"full":false,"thumbnail":false,"medium":false,"medium_large":false,"large":false,"twp-icon":false,"1536x1536":false,"2048x2048":false},"uagb_author_info":{"display_name":"\u9ec3\u9806\u8208","author_link":"\/phys\/?author=10"},"uagb_comment_info":0,"uagb_excerpt":"\u59d3\u540d\uff1a\u5289\u91c7\u9748\uff0c\u6307\u5c0e\u6559\u6388\uff1a\u675c\u662d\u5b8f","_links":{"self":[{"href":"\/phys\/index.php?rest_route=\/wp\/v2\/pages\/27336"}],"collection":[{"href":"\/phys\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"\/phys\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"\/phys\/index.php?rest_route=\/wp\/v2\/users\/10"}],"replies":[{"embeddable":true,"href":"\/phys\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=27336"}],"version-history":[{"count":3,"href":"\/phys\/index.php?rest_route=\/wp\/v2\/pages\/27336\/revisions"}],"predecessor-version":[{"id":27501,"href":"\/phys\/index.php?rest_route=\/wp\/v2\/pages\/27336\/revisions\/27501"}],"wp:attachment":[{"href":"\/phys\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=27336"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}