Fluctuation conductivity of polycrystalline Hg, Tl-1223

Detailed resistivity measurements were made for polycrystalline Hg1−xTlxBa2Ca2Cu3O8+δ (x=0 and 0.2) in zero field and above the superconducting Tc. The fluctuation conductivity Δσ is analyzed. With decreasing temperature two crossover temperatures could be identified for each sample; i.e. T∗ from tw...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Physica. C, Superconductivity Superconductivity, 2003-05, Vol.388-389, p.349-350
Hauptverfasser: Han, S.H, Bryntse, I, Axnäs, J, Zhao, B.R, Rapp, Ö
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 350
container_issue
container_start_page 349
container_title Physica. C, Superconductivity
container_volume 388-389
creator Han, S.H
Bryntse, I
Axnäs, J
Zhao, B.R
Rapp, Ö
description Detailed resistivity measurements were made for polycrystalline Hg1−xTlxBa2Ca2Cu3O8+δ (x=0 and 0.2) in zero field and above the superconducting Tc. The fluctuation conductivity Δσ is analyzed. With decreasing temperature two crossover temperatures could be identified for each sample; i.e. T∗ from two to three dimensional fluctuations in the mean field region (MFR), and TG from the MFR to the critical region. All results are in agreement with the Lawrence–Doniach model. The c-axis coherence length and the interlayer coupling factor were obtained.
doi_str_mv 10.1016/S0921-4534(02)02497-8
format Article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_27882223</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0921453402024978</els_id><sourcerecordid>27882223</sourcerecordid><originalsourceid>FETCH-LOGICAL-c338t-10830c0fe5751319ba0fc311bb0b0d80abfad62f915d61776f5548c1dde39d893</originalsourceid><addsrcrecordid>eNqFkE9LAzEQxYMoWKsfQdiTKLg6k-x2syeRYq1Q8GA9h2z-SCTd1GS3sN_erRWvzmUYeO8x70fIJcIdAs7u36CmmBclK66B3gAt6irnR2SCvGI5xYIdk8mf5JScpfQJ42CNE1ItfK-6XnYutJkKrR4vt3PdkAWbbYMfVBxSJ713rcmWH7fZ2udIKTsnJ1b6ZC5-95S8L57W82W-en1-mT-ucsUY73IEzkCBNWVVIsO6kWAVQ2waaEBzkI2VekZtjaWeYVXNbFkWXKHWhtWa12xKrg652xi-epM6sXFJGe9la0KfBK04p-M_o7A8CFUMKUVjxTa6jYyDQBB7TOIHk9gzEEDFDybBR9_DwWfGFjtnokjKmVYZ7aJRndDB_ZPwDU33bdc</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>27882223</pqid></control><display><type>article</type><title>Fluctuation conductivity of polycrystalline Hg, Tl-1223</title><source>ScienceDirect Journals (5 years ago - present)</source><creator>Han, S.H ; Bryntse, I ; Axnäs, J ; Zhao, B.R ; Rapp, Ö</creator><creatorcontrib>Han, S.H ; Bryntse, I ; Axnäs, J ; Zhao, B.R ; Rapp, Ö</creatorcontrib><description>Detailed resistivity measurements were made for polycrystalline Hg1−xTlxBa2Ca2Cu3O8+δ (x=0 and 0.2) in zero field and above the superconducting Tc. The fluctuation conductivity Δσ is analyzed. With decreasing temperature two crossover temperatures could be identified for each sample; i.e. T∗ from two to three dimensional fluctuations in the mean field region (MFR), and TG from the MFR to the critical region. All results are in agreement with the Lawrence–Doniach model. The c-axis coherence length and the interlayer coupling factor were obtained.</description><identifier>ISSN: 0921-4534</identifier><identifier>EISSN: 1873-2143</identifier><identifier>DOI: 10.1016/S0921-4534(02)02497-8</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Fluctuation conductivity ; Hg, Tl-1223</subject><ispartof>Physica. C, Superconductivity, 2003-05, Vol.388-389, p.349-350</ispartof><rights>2003 Elsevier Science B.V.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c338t-10830c0fe5751319ba0fc311bb0b0d80abfad62f915d61776f5548c1dde39d893</citedby><cites>FETCH-LOGICAL-c338t-10830c0fe5751319ba0fc311bb0b0d80abfad62f915d61776f5548c1dde39d893</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/S0921-4534(02)02497-8$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3548,27922,27923,45993</link.rule.ids></links><search><creatorcontrib>Han, S.H</creatorcontrib><creatorcontrib>Bryntse, I</creatorcontrib><creatorcontrib>Axnäs, J</creatorcontrib><creatorcontrib>Zhao, B.R</creatorcontrib><creatorcontrib>Rapp, Ö</creatorcontrib><title>Fluctuation conductivity of polycrystalline Hg, Tl-1223</title><title>Physica. C, Superconductivity</title><description>Detailed resistivity measurements were made for polycrystalline Hg1−xTlxBa2Ca2Cu3O8+δ (x=0 and 0.2) in zero field and above the superconducting Tc. The fluctuation conductivity Δσ is analyzed. With decreasing temperature two crossover temperatures could be identified for each sample; i.e. T∗ from two to three dimensional fluctuations in the mean field region (MFR), and TG from the MFR to the critical region. All results are in agreement with the Lawrence–Doniach model. The c-axis coherence length and the interlayer coupling factor were obtained.</description><subject>Fluctuation conductivity</subject><subject>Hg, Tl-1223</subject><issn>0921-4534</issn><issn>1873-2143</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2003</creationdate><recordtype>article</recordtype><recordid>eNqFkE9LAzEQxYMoWKsfQdiTKLg6k-x2syeRYq1Q8GA9h2z-SCTd1GS3sN_erRWvzmUYeO8x70fIJcIdAs7u36CmmBclK66B3gAt6irnR2SCvGI5xYIdk8mf5JScpfQJ42CNE1ItfK-6XnYutJkKrR4vt3PdkAWbbYMfVBxSJ713rcmWH7fZ2udIKTsnJ1b6ZC5-95S8L57W82W-en1-mT-ucsUY73IEzkCBNWVVIsO6kWAVQ2waaEBzkI2VekZtjaWeYVXNbFkWXKHWhtWa12xKrg652xi-epM6sXFJGe9la0KfBK04p-M_o7A8CFUMKUVjxTa6jYyDQBB7TOIHk9gzEEDFDybBR9_DwWfGFjtnokjKmVYZ7aJRndDB_ZPwDU33bdc</recordid><startdate>200305</startdate><enddate>200305</enddate><creator>Han, S.H</creator><creator>Bryntse, I</creator><creator>Axnäs, J</creator><creator>Zhao, B.R</creator><creator>Rapp, Ö</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>200305</creationdate><title>Fluctuation conductivity of polycrystalline Hg, Tl-1223</title><author>Han, S.H ; Bryntse, I ; Axnäs, J ; Zhao, B.R ; Rapp, Ö</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c338t-10830c0fe5751319ba0fc311bb0b0d80abfad62f915d61776f5548c1dde39d893</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2003</creationdate><topic>Fluctuation conductivity</topic><topic>Hg, Tl-1223</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Han, S.H</creatorcontrib><creatorcontrib>Bryntse, I</creatorcontrib><creatorcontrib>Axnäs, J</creatorcontrib><creatorcontrib>Zhao, B.R</creatorcontrib><creatorcontrib>Rapp, Ö</creatorcontrib><collection>CrossRef</collection><collection>Electronics &amp; Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</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>Han, S.H</au><au>Bryntse, I</au><au>Axnäs, J</au><au>Zhao, B.R</au><au>Rapp, Ö</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Fluctuation conductivity of polycrystalline Hg, Tl-1223</atitle><jtitle>Physica. C, Superconductivity</jtitle><date>2003-05</date><risdate>2003</risdate><volume>388-389</volume><spage>349</spage><epage>350</epage><pages>349-350</pages><issn>0921-4534</issn><eissn>1873-2143</eissn><abstract>Detailed resistivity measurements were made for polycrystalline Hg1−xTlxBa2Ca2Cu3O8+δ (x=0 and 0.2) in zero field and above the superconducting Tc. The fluctuation conductivity Δσ is analyzed. With decreasing temperature two crossover temperatures could be identified for each sample; i.e. T∗ from two to three dimensional fluctuations in the mean field region (MFR), and TG from the MFR to the critical region. All results are in agreement with the Lawrence–Doniach model. The c-axis coherence length and the interlayer coupling factor were obtained.</abstract><pub>Elsevier B.V</pub><doi>10.1016/S0921-4534(02)02497-8</doi><tpages>2</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0921-4534
ispartof Physica. C, Superconductivity, 2003-05, Vol.388-389, p.349-350
issn 0921-4534
1873-2143
language eng
recordid cdi_proquest_miscellaneous_27882223
source ScienceDirect Journals (5 years ago - present)
subjects Fluctuation conductivity
Hg, Tl-1223
title Fluctuation conductivity of polycrystalline Hg, Tl-1223
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-13T21%3A12%3A35IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Fluctuation%20conductivity%20of%20polycrystalline%20Hg,%20Tl-1223&rft.jtitle=Physica.%20C,%20Superconductivity&rft.au=Han,%20S.H&rft.date=2003-05&rft.volume=388-389&rft.spage=349&rft.epage=350&rft.pages=349-350&rft.issn=0921-4534&rft.eissn=1873-2143&rft_id=info:doi/10.1016/S0921-4534(02)02497-8&rft_dat=%3Cproquest_cross%3E27882223%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=27882223&rft_id=info:pmid/&rft_els_id=S0921453402024978&rfr_iscdi=true