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Electron Number-Based Phase Diagram of Pr sub(1-x) LaCe sub(x) CuO sub(4-[delta]) and Possible Absence of Disparity between Electron- and Hole-Doped Cuprate Phase Diagrams
We performed annealing and angle resolved photoemission spectroscopy studies on electron-doped cuprate Pr sub(1-x) LaCe sub(x) CuO sub(4-[delta])(PLCCO). It is found that the optimal annealing condition is dependent on the Ce content x. The electron number (n) is estimated from the experimentally ob...
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Published in: | Physical review letters 2017-03, Vol.118 (13) |
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creator | Song, Dongjoon Han, Garam Kyung, Wonshik Seo, Jeongjin Cho, Soohyun Kim, Beom Seo Arita, Masashi Shimada, Kenya Namatame, Hirofumi Taniguchi, Masaki Yoshida, Y Eisaki, H Park, Seung Ryong Kim, C |
description | We performed annealing and angle resolved photoemission spectroscopy studies on electron-doped cuprate Pr sub(1-x) LaCe sub(x) CuO sub(4-[delta])(PLCCO). It is found that the optimal annealing condition is dependent on the Ce content x. The electron number (n) is estimated from the experimentally obtained Fermi surface volume for x= 0.10, 0.15 and 0.18 samples. It clearly shows a significant and annealing dependent deviation from the nominal x. In addition, we observe that the pseudo-gap at hot spots is also closely correlated with n; the pseudogap gradually closes as n increases. We established a new phase diagram of PLCCO as a function of n. Different from the x-based one, the new phase diagram shows similar antiferromagnetic and superconducting phases to those of hole doped ones. Our results raise a possibility for absence of disparity between the phase diagrams of electron- and hole-doped cuprates |
doi_str_mv | 10.1103/PhysRevLett.118.137001 |
format | article |
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It is found that the optimal annealing condition is dependent on the Ce content x. The electron number (n) is estimated from the experimentally obtained Fermi surface volume for x= 0.10, 0.15 and 0.18 samples. It clearly shows a significant and annealing dependent deviation from the nominal x. In addition, we observe that the pseudo-gap at hot spots is also closely correlated with n; the pseudogap gradually closes as n increases. We established a new phase diagram of PLCCO as a function of n. Different from the x-based one, the new phase diagram shows similar antiferromagnetic and superconducting phases to those of hole doped ones. Our results raise a possibility for absence of disparity between the phase diagrams of electron- and hole-doped cuprates</description><identifier>ISSN: 0031-9007</identifier><identifier>EISSN: 1079-7114</identifier><identifier>DOI: 10.1103/PhysRevLett.118.137001</identifier><language>eng</language><subject>Annealing ; ANNEALING PROCESSES ; COPPER OXIDE ; Correlation ; Cuprates ; Deviation ; DOPING ; HOLES ; Hot spots ; MAGNETIC PROPERTIES ; Optimization ; Phase diagrams ; PHASES ; SUPERCONDUCTIVITY</subject><ispartof>Physical review letters, 2017-03, Vol.118 (13)</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Song, Dongjoon</creatorcontrib><creatorcontrib>Han, Garam</creatorcontrib><creatorcontrib>Kyung, Wonshik</creatorcontrib><creatorcontrib>Seo, Jeongjin</creatorcontrib><creatorcontrib>Cho, Soohyun</creatorcontrib><creatorcontrib>Kim, Beom Seo</creatorcontrib><creatorcontrib>Arita, Masashi</creatorcontrib><creatorcontrib>Shimada, Kenya</creatorcontrib><creatorcontrib>Namatame, Hirofumi</creatorcontrib><creatorcontrib>Taniguchi, Masaki</creatorcontrib><creatorcontrib>Yoshida, Y</creatorcontrib><creatorcontrib>Eisaki, H</creatorcontrib><creatorcontrib>Park, Seung Ryong</creatorcontrib><creatorcontrib>Kim, C</creatorcontrib><title>Electron Number-Based Phase Diagram of Pr sub(1-x) LaCe sub(x) CuO sub(4-[delta]) and Possible Absence of Disparity between Electron- and Hole-Doped Cuprate Phase Diagrams</title><title>Physical review letters</title><description>We performed annealing and angle resolved photoemission spectroscopy studies on electron-doped cuprate Pr sub(1-x) LaCe sub(x) CuO sub(4-[delta])(PLCCO). It is found that the optimal annealing condition is dependent on the Ce content x. The electron number (n) is estimated from the experimentally obtained Fermi surface volume for x= 0.10, 0.15 and 0.18 samples. It clearly shows a significant and annealing dependent deviation from the nominal x. In addition, we observe that the pseudo-gap at hot spots is also closely correlated with n; the pseudogap gradually closes as n increases. We established a new phase diagram of PLCCO as a function of n. Different from the x-based one, the new phase diagram shows similar antiferromagnetic and superconducting phases to those of hole doped ones. Our results raise a possibility for absence of disparity between the phase diagrams of electron- and hole-doped cuprates</description><subject>Annealing</subject><subject>ANNEALING PROCESSES</subject><subject>COPPER OXIDE</subject><subject>Correlation</subject><subject>Cuprates</subject><subject>Deviation</subject><subject>DOPING</subject><subject>HOLES</subject><subject>Hot spots</subject><subject>MAGNETIC PROPERTIES</subject><subject>Optimization</subject><subject>Phase diagrams</subject><subject>PHASES</subject><subject>SUPERCONDUCTIVITY</subject><issn>0031-9007</issn><issn>1079-7114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNqVTstOwzAQtBBIhMcvIB_bg4udRE1yhKSohwoixA2hykm3NMixg9cG-k38JCaCA0dOM7OaxxJyIfhMCJ5c1rs93sPbCpwLh3wmkoxzcUAiwbOCZUKkhyTiPBGs4Dw7JieILzw44nkekc-FgtZZo-mt7xuw7FoibGi9C0CrTj5b2VOzpbWl6JuJYB9TupIljCrw0t-NNGWPG1BOPk2p1CFvELtGAb1qEHQL3xVVh4O0ndvTBtw7gKa_22zMLI0CVpkhzJd-sNLB3zfwjBxtpUI4_8FTMrlZPJRLNljz6gHduu-wBaWkBuNxLQqexnGaz7PkH9Yv765qDw</recordid><startdate>20170331</startdate><enddate>20170331</enddate><creator>Song, Dongjoon</creator><creator>Han, Garam</creator><creator>Kyung, Wonshik</creator><creator>Seo, Jeongjin</creator><creator>Cho, Soohyun</creator><creator>Kim, Beom Seo</creator><creator>Arita, Masashi</creator><creator>Shimada, Kenya</creator><creator>Namatame, Hirofumi</creator><creator>Taniguchi, Masaki</creator><creator>Yoshida, Y</creator><creator>Eisaki, H</creator><creator>Park, Seung Ryong</creator><creator>Kim, C</creator><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>H8G</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20170331</creationdate><title>Electron Number-Based Phase Diagram of Pr sub(1-x) LaCe sub(x) CuO sub(4-[delta]) and Possible Absence of Disparity between Electron- and Hole-Doped Cuprate Phase Diagrams</title><author>Song, Dongjoon ; Han, Garam ; Kyung, Wonshik ; Seo, Jeongjin ; Cho, Soohyun ; Kim, Beom Seo ; Arita, Masashi ; Shimada, Kenya ; Namatame, Hirofumi ; Taniguchi, Masaki ; Yoshida, Y ; Eisaki, H ; Park, Seung Ryong ; Kim, C</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_19042248673</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Annealing</topic><topic>ANNEALING PROCESSES</topic><topic>COPPER OXIDE</topic><topic>Correlation</topic><topic>Cuprates</topic><topic>Deviation</topic><topic>DOPING</topic><topic>HOLES</topic><topic>Hot spots</topic><topic>MAGNETIC PROPERTIES</topic><topic>Optimization</topic><topic>Phase diagrams</topic><topic>PHASES</topic><topic>SUPERCONDUCTIVITY</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Song, Dongjoon</creatorcontrib><creatorcontrib>Han, Garam</creatorcontrib><creatorcontrib>Kyung, Wonshik</creatorcontrib><creatorcontrib>Seo, Jeongjin</creatorcontrib><creatorcontrib>Cho, Soohyun</creatorcontrib><creatorcontrib>Kim, Beom Seo</creatorcontrib><creatorcontrib>Arita, Masashi</creatorcontrib><creatorcontrib>Shimada, Kenya</creatorcontrib><creatorcontrib>Namatame, Hirofumi</creatorcontrib><creatorcontrib>Taniguchi, Masaki</creatorcontrib><creatorcontrib>Yoshida, Y</creatorcontrib><creatorcontrib>Eisaki, H</creatorcontrib><creatorcontrib>Park, Seung Ryong</creatorcontrib><creatorcontrib>Kim, C</creatorcontrib><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Copper Technical Reference Library</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Song, Dongjoon</au><au>Han, Garam</au><au>Kyung, Wonshik</au><au>Seo, Jeongjin</au><au>Cho, Soohyun</au><au>Kim, Beom Seo</au><au>Arita, Masashi</au><au>Shimada, Kenya</au><au>Namatame, Hirofumi</au><au>Taniguchi, Masaki</au><au>Yoshida, Y</au><au>Eisaki, H</au><au>Park, Seung Ryong</au><au>Kim, C</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electron Number-Based Phase Diagram of Pr sub(1-x) LaCe sub(x) CuO sub(4-[delta]) and Possible Absence of Disparity between Electron- and Hole-Doped Cuprate Phase Diagrams</atitle><jtitle>Physical review letters</jtitle><date>2017-03-31</date><risdate>2017</risdate><volume>118</volume><issue>13</issue><issn>0031-9007</issn><eissn>1079-7114</eissn><abstract>We performed annealing and angle resolved photoemission spectroscopy studies on electron-doped cuprate Pr sub(1-x) LaCe sub(x) CuO sub(4-[delta])(PLCCO). It is found that the optimal annealing condition is dependent on the Ce content x. The electron number (n) is estimated from the experimentally obtained Fermi surface volume for x= 0.10, 0.15 and 0.18 samples. It clearly shows a significant and annealing dependent deviation from the nominal x. In addition, we observe that the pseudo-gap at hot spots is also closely correlated with n; the pseudogap gradually closes as n increases. We established a new phase diagram of PLCCO as a function of n. Different from the x-based one, the new phase diagram shows similar antiferromagnetic and superconducting phases to those of hole doped ones. Our results raise a possibility for absence of disparity between the phase diagrams of electron- and hole-doped cuprates</abstract><doi>10.1103/PhysRevLett.118.137001</doi></addata></record> |
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source | American Physical Society:Jisc Collections:APS Read and Publish 2023-2025 (reading list) |
subjects | Annealing ANNEALING PROCESSES COPPER OXIDE Correlation Cuprates Deviation DOPING HOLES Hot spots MAGNETIC PROPERTIES Optimization Phase diagrams PHASES SUPERCONDUCTIVITY |
title | Electron Number-Based Phase Diagram of Pr sub(1-x) LaCe sub(x) CuO sub(4-[delta]) and Possible Absence of Disparity between Electron- and Hole-Doped Cuprate Phase Diagrams |
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