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Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution
Lead substitutions on Hg site and Ca substitutions on Y site have been studied in the Hg-2212 compound in order to reach its optimal doping composition. The unit cell evolution has been studied by powder X-ray diffraction and the structure refined from X-ray synchrotron powder diffraction data. The...
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Published in: | Physica. C, Superconductivity Superconductivity, 2002-01, Vol.366 (3), p.147-156 |
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container_title | Physica. C, Superconductivity |
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creator | Toulemonde, P Odier, P Bordet, P Bruyère, R Tholence, J.L |
description | Lead substitutions on Hg site and Ca substitutions on Y site have been studied in the Hg-2212 compound in order to reach its optimal doping composition. The unit cell evolution has been studied by powder X-ray diffraction and the structure refined from X-ray synchrotron powder diffraction data. The Pb
4+ substitution stabilizes the Hg
2O
2−
δ
layer allowing full Ca substitution on the Y site. The Ca doping makes the Ba–O2 plane to move away from the Hg–O3 plane, it also reduces the buckling which remains still high (9.7°). The superconducting transitions correspond to optimally and overdoped samples. The
T
c
max
(82–84 K) is found identical as in (Hg,Tl)-2212 samples suggesting this value to be intrinsic at optimal doping. |
doi_str_mv | 10.1016/S0921-4534(01)00908-X |
format | article |
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4+ substitution stabilizes the Hg
2O
2−
δ
layer allowing full Ca substitution on the Y site. The Ca doping makes the Ba–O2 plane to move away from the Hg–O3 plane, it also reduces the buckling which remains still high (9.7°). The superconducting transitions correspond to optimally and overdoped samples. The
T
c
max
(82–84 K) is found identical as in (Hg,Tl)-2212 samples suggesting this value to be intrinsic at optimal doping.</description><identifier>ISSN: 0921-4534</identifier><identifier>EISSN: 1873-2143</identifier><identifier>DOI: 10.1016/S0921-4534(01)00908-X</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Crystal structure ; High-pressure high-temperature synthesis ; Mercury-based high- Tc superconductors ; Synchrotron X-ray powder diffraction</subject><ispartof>Physica. C, Superconductivity, 2002-01, Vol.366 (3), p.147-156</ispartof><rights>2002 Elsevier Science B.V.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c369t-7414453c093748907e435535734b26f4a0dc9a86c5752419a3af2998ddf284503</citedby><cites>FETCH-LOGICAL-c369t-7414453c093748907e435535734b26f4a0dc9a86c5752419a3af2998ddf284503</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Toulemonde, P</creatorcontrib><creatorcontrib>Odier, P</creatorcontrib><creatorcontrib>Bordet, P</creatorcontrib><creatorcontrib>Bruyère, R</creatorcontrib><creatorcontrib>Tholence, J.L</creatorcontrib><title>Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution</title><title>Physica. C, Superconductivity</title><description>Lead substitutions on Hg site and Ca substitutions on Y site have been studied in the Hg-2212 compound in order to reach its optimal doping composition. The unit cell evolution has been studied by powder X-ray diffraction and the structure refined from X-ray synchrotron powder diffraction data. The Pb
4+ substitution stabilizes the Hg
2O
2−
δ
layer allowing full Ca substitution on the Y site. The Ca doping makes the Ba–O2 plane to move away from the Hg–O3 plane, it also reduces the buckling which remains still high (9.7°). The superconducting transitions correspond to optimally and overdoped samples. The
T
c
max
(82–84 K) is found identical as in (Hg,Tl)-2212 samples suggesting this value to be intrinsic at optimal doping.</description><subject>Crystal structure</subject><subject>High-pressure high-temperature synthesis</subject><subject>Mercury-based high- Tc superconductors</subject><subject>Synchrotron X-ray powder diffraction</subject><issn>0921-4534</issn><issn>1873-2143</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2002</creationdate><recordtype>article</recordtype><recordid>eNqNkMtKAzEUhoMoWKuPIGQluhjNdWayEilqhULFC3QXZpIzJTI3k0yhb-_Uils9m7P5_p9zPoTOKbmmhKY3r0QxmgjJxSWhV4QokierAzShecYTRgU_RJNf5BidhPBBxqGKTtDLso-uKWpctBZ3G_C268HiMPTgTdfawUTXrrGHtWsgYNfi-TphjDIctiFCg8stfi5HvgzRxSG6rj1FR1VRBzj72VP0_nD_Npsni-Xj0-xukRieqphkgorxIEMUz0SuSAaCS8llxkXJ0koUxBpV5KmRmWSCqoIXFVMqt7ZiuZCET9HFvrf33ecAIerGBQN1XbTQDUGzLM1kKvl_wJQywkZQ7kHjuxA8VLr3oxy_1ZTonWr9rVrvPGpC9bdqvRpzt_scjO9uHHgdjIPWgHUeTNS2c380fAGFboQo</recordid><startdate>20020115</startdate><enddate>20020115</enddate><creator>Toulemonde, P</creator><creator>Odier, P</creator><creator>Bordet, P</creator><creator>Bruyère, R</creator><creator>Tholence, J.L</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7QQ</scope><scope>8FD</scope><scope>JG9</scope><scope>7U5</scope><scope>L7M</scope></search><sort><creationdate>20020115</creationdate><title>Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution</title><author>Toulemonde, P ; Odier, P ; Bordet, P ; Bruyère, R ; Tholence, J.L</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c369t-7414453c093748907e435535734b26f4a0dc9a86c5752419a3af2998ddf284503</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2002</creationdate><topic>Crystal structure</topic><topic>High-pressure high-temperature synthesis</topic><topic>Mercury-based high- Tc superconductors</topic><topic>Synchrotron X-ray powder diffraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Toulemonde, P</creatorcontrib><creatorcontrib>Odier, P</creatorcontrib><creatorcontrib>Bordet, P</creatorcontrib><creatorcontrib>Bruyère, R</creatorcontrib><creatorcontrib>Tholence, J.L</creatorcontrib><collection>CrossRef</collection><collection>Ceramic Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physica. C, Superconductivity</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Toulemonde, P</au><au>Odier, P</au><au>Bordet, P</au><au>Bruyère, R</au><au>Tholence, J.L</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution</atitle><jtitle>Physica. C, Superconductivity</jtitle><date>2002-01-15</date><risdate>2002</risdate><volume>366</volume><issue>3</issue><spage>147</spage><epage>156</epage><pages>147-156</pages><issn>0921-4534</issn><eissn>1873-2143</eissn><abstract>Lead substitutions on Hg site and Ca substitutions on Y site have been studied in the Hg-2212 compound in order to reach its optimal doping composition. The unit cell evolution has been studied by powder X-ray diffraction and the structure refined from X-ray synchrotron powder diffraction data. The Pb
4+ substitution stabilizes the Hg
2O
2−
δ
layer allowing full Ca substitution on the Y site. The Ca doping makes the Ba–O2 plane to move away from the Hg–O3 plane, it also reduces the buckling which remains still high (9.7°). The superconducting transitions correspond to optimally and overdoped samples. The
T
c
max
(82–84 K) is found identical as in (Hg,Tl)-2212 samples suggesting this value to be intrinsic at optimal doping.</abstract><pub>Elsevier B.V</pub><doi>10.1016/S0921-4534(01)00908-X</doi><tpages>10</tpages></addata></record> |
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source | ScienceDirect Freedom Collection |
subjects | Crystal structure High-pressure high-temperature synthesis Mercury-based high- Tc superconductors Synchrotron X-ray powder diffraction |
title | Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution |
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