Effect of Gd addition on the activation energies of Bi-2223 superconductor
We have investigated the effect of addition of Gd in Bi 1.8Pb 0.35Sr 1.9Ca 2.1Cu 3Gd x O y superconductor with x=0, 0.1, 0.2, 0.3, 0.4 and 0.5. The samples were prepared using the standard solid-state reaction method. The activation energies, irreversibility fields ( H irr), upper critical fields (...
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Veröffentlicht in: | Physica. B, Condensed matter Condensed matter, 2011-02, Vol.406 (3), p.705-709 |
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container_title | Physica. B, Condensed matter |
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creator | Erdem, M. Özturk, Ö. Yucel, E. Altintas, S.P. Varilci, A. Terzioğlu, C. Belenli, I. |
description | We have investigated the effect of addition of Gd in Bi
1.8Pb
0.35Sr
1.9Ca
2.1Cu
3Gd
x
O
y
superconductor with
x=0, 0.1, 0.2, 0.3, 0.4 and 0.5. The samples were prepared using the standard solid-state reaction method. The activation energies, irreversibility fields (
H
irr), upper critical fields (
H
c2) and coherence lengths at 0
K (
ξ(0)) were calculated from the resistivity versus temperature (
R–
T) curves under DC magnetic fields up to 7
T. The superconducting transition temperature,
T
c, and activation energy,
U
0, were found to decrease with increase in Gd concentration and with increase in applied magnetic field. The offset transition temperature of the pure (Gd00) sample without applied magnetic field is 108
K, whereas for Gd05 sample, the offset transition temperature drops to 5
K with 7
T applied magnetic field. The activation energy of the Gd00 sample without applied magnetic field is 34,980
K, and for Gd05 sample with 7
T applied field it is 98
K.
H
irr and
H
c2 values also decrease with increase in Gd addition. The possible reasons for the observed degradation in microstructural and superconducting properties due to Gd addition were discussed. |
doi_str_mv | 10.1016/j.physb.2010.12.008 |
format | Article |
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1.8Pb
0.35Sr
1.9Ca
2.1Cu
3Gd
x
O
y
superconductor with
x=0, 0.1, 0.2, 0.3, 0.4 and 0.5. The samples were prepared using the standard solid-state reaction method. The activation energies, irreversibility fields (
H
irr), upper critical fields (
H
c2) and coherence lengths at 0
K (
ξ(0)) were calculated from the resistivity versus temperature (
R–
T) curves under DC magnetic fields up to 7
T. The superconducting transition temperature,
T
c, and activation energy,
U
0, were found to decrease with increase in Gd concentration and with increase in applied magnetic field. The offset transition temperature of the pure (Gd00) sample without applied magnetic field is 108
K, whereas for Gd05 sample, the offset transition temperature drops to 5
K with 7
T applied magnetic field. The activation energy of the Gd00 sample without applied magnetic field is 34,980
K, and for Gd05 sample with 7
T applied field it is 98
K.
H
irr and
H
c2 values also decrease with increase in Gd addition. The possible reasons for the observed degradation in microstructural and superconducting properties due to Gd addition were discussed.</description><identifier>ISSN: 0921-4526</identifier><identifier>EISSN: 1873-2135</identifier><identifier>DOI: 10.1016/j.physb.2010.12.008</identifier><language>eng</language><publisher>Kidlington: Elsevier B.V</publisher><subject>ACTIVATION ENERGY ; BSCCO-2223 ; Condensed matter ; Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Effects of crystal defects, doping and substitution ; ELECTRICAL CONDUCTIVITY ; Electrical resistivity ; Exact sciences and technology ; High temperature superconductors ; MAGNETIC FIELD ; Magnetic fields ; MATHEMATICAL ANALYSIS ; Mixed state, critical fields, and surface sheath ; Offsets ; Physics ; Properties of type I and type II superconductors ; Rare earth addition ; SUPERCONDUCTIVITY ; SUPERCONDUCTORS ; TRANSITION TEMPERATURE ; Transition temperature variations</subject><ispartof>Physica. B, Condensed matter, 2011-02, Vol.406 (3), p.705-709</ispartof><rights>2010 Elsevier B.V.</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c365t-8706364069907628036b50f49d3f7d8eb1acd72b3ad11ed5011f7412ee2c5d6c3</citedby><cites>FETCH-LOGICAL-c365t-8706364069907628036b50f49d3f7d8eb1acd72b3ad11ed5011f7412ee2c5d6c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.physb.2010.12.008$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>315,782,786,3554,27933,27934,46004</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=23789711$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Erdem, M.</creatorcontrib><creatorcontrib>Özturk, Ö.</creatorcontrib><creatorcontrib>Yucel, E.</creatorcontrib><creatorcontrib>Altintas, S.P.</creatorcontrib><creatorcontrib>Varilci, A.</creatorcontrib><creatorcontrib>Terzioğlu, C.</creatorcontrib><creatorcontrib>Belenli, I.</creatorcontrib><title>Effect of Gd addition on the activation energies of Bi-2223 superconductor</title><title>Physica. B, Condensed matter</title><description>We have investigated the effect of addition of Gd in Bi
1.8Pb
0.35Sr
1.9Ca
2.1Cu
3Gd
x
O
y
superconductor with
x=0, 0.1, 0.2, 0.3, 0.4 and 0.5. The samples were prepared using the standard solid-state reaction method. The activation energies, irreversibility fields (
H
irr), upper critical fields (
H
c2) and coherence lengths at 0
K (
ξ(0)) were calculated from the resistivity versus temperature (
R–
T) curves under DC magnetic fields up to 7
T. The superconducting transition temperature,
T
c, and activation energy,
U
0, were found to decrease with increase in Gd concentration and with increase in applied magnetic field. The offset transition temperature of the pure (Gd00) sample without applied magnetic field is 108
K, whereas for Gd05 sample, the offset transition temperature drops to 5
K with 7
T applied magnetic field. The activation energy of the Gd00 sample without applied magnetic field is 34,980
K, and for Gd05 sample with 7
T applied field it is 98
K.
H
irr and
H
c2 values also decrease with increase in Gd addition. The possible reasons for the observed degradation in microstructural and superconducting properties due to Gd addition were discussed.</description><subject>ACTIVATION ENERGY</subject><subject>BSCCO-2223</subject><subject>Condensed matter</subject><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Effects of crystal defects, doping and substitution</subject><subject>ELECTRICAL CONDUCTIVITY</subject><subject>Electrical resistivity</subject><subject>Exact sciences and technology</subject><subject>High temperature superconductors</subject><subject>MAGNETIC FIELD</subject><subject>Magnetic fields</subject><subject>MATHEMATICAL ANALYSIS</subject><subject>Mixed state, critical fields, and surface sheath</subject><subject>Offsets</subject><subject>Physics</subject><subject>Properties of type I and type II superconductors</subject><subject>Rare earth addition</subject><subject>SUPERCONDUCTIVITY</subject><subject>SUPERCONDUCTORS</subject><subject>TRANSITION TEMPERATURE</subject><subject>Transition temperature variations</subject><issn>0921-4526</issn><issn>1873-2135</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNp9kDFPwzAQhS0EEqXwC1iyIKYUn53YycAAVSmgSiwwW459pq7SpNhppf57krZi5HTSSaf33uk-Qm6BToCCeFhNNst9rCaMDhs2obQ4IyMoJE8Z8PycjGjJIM1yJi7JVYwr2hdIGJH3mXNouqR1ydwm2lrf-bZJ-u6WmGjT-Z0-bLDB8O0xDspnnzLGeBK3GwymbezWdG24JhdO1xFvTnNMvl5mn9PXdPExf5s-LVLDRd6lhaSCi4yKsqRSsIJyUeXUZaXlTtoCK9DGSlZxbQHQ5hTAyQwYIjO5FYaPyf0xdxPany3GTq19NFjXusF2G1WR5xKAZ1mv5EelCW2MAZ3aBL_WYa-AqgGcWqkDODWAU8BUD6533Z3ydTS6dkE3xsc_K-OyKIcDY_J41GH_7M5jUNF4bAxaH3qkyrb-3zu_kxeC5A</recordid><startdate>20110201</startdate><enddate>20110201</enddate><creator>Erdem, M.</creator><creator>Özturk, Ö.</creator><creator>Yucel, E.</creator><creator>Altintas, S.P.</creator><creator>Varilci, A.</creator><creator>Terzioğlu, C.</creator><creator>Belenli, I.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>H8G</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20110201</creationdate><title>Effect of Gd addition on the activation energies of Bi-2223 superconductor</title><author>Erdem, M. ; Özturk, Ö. ; Yucel, E. ; Altintas, S.P. ; Varilci, A. ; Terzioğlu, C. ; Belenli, I.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c365t-8706364069907628036b50f49d3f7d8eb1acd72b3ad11ed5011f7412ee2c5d6c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>ACTIVATION ENERGY</topic><topic>BSCCO-2223</topic><topic>Condensed matter</topic><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Effects of crystal defects, doping and substitution</topic><topic>ELECTRICAL CONDUCTIVITY</topic><topic>Electrical resistivity</topic><topic>Exact sciences and technology</topic><topic>High temperature superconductors</topic><topic>MAGNETIC FIELD</topic><topic>Magnetic fields</topic><topic>MATHEMATICAL ANALYSIS</topic><topic>Mixed state, critical fields, and surface sheath</topic><topic>Offsets</topic><topic>Physics</topic><topic>Properties of type I and type II superconductors</topic><topic>Rare earth addition</topic><topic>SUPERCONDUCTIVITY</topic><topic>SUPERCONDUCTORS</topic><topic>TRANSITION TEMPERATURE</topic><topic>Transition temperature variations</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Erdem, M.</creatorcontrib><creatorcontrib>Özturk, Ö.</creatorcontrib><creatorcontrib>Yucel, E.</creatorcontrib><creatorcontrib>Altintas, S.P.</creatorcontrib><creatorcontrib>Varilci, A.</creatorcontrib><creatorcontrib>Terzioğlu, C.</creatorcontrib><creatorcontrib>Belenli, I.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Copper Technical Reference Library</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physica. B, Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Erdem, M.</au><au>Özturk, Ö.</au><au>Yucel, E.</au><au>Altintas, S.P.</au><au>Varilci, A.</au><au>Terzioğlu, C.</au><au>Belenli, I.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of Gd addition on the activation energies of Bi-2223 superconductor</atitle><jtitle>Physica. B, Condensed matter</jtitle><date>2011-02-01</date><risdate>2011</risdate><volume>406</volume><issue>3</issue><spage>705</spage><epage>709</epage><pages>705-709</pages><issn>0921-4526</issn><eissn>1873-2135</eissn><abstract>We have investigated the effect of addition of Gd in Bi
1.8Pb
0.35Sr
1.9Ca
2.1Cu
3Gd
x
O
y
superconductor with
x=0, 0.1, 0.2, 0.3, 0.4 and 0.5. The samples were prepared using the standard solid-state reaction method. The activation energies, irreversibility fields (
H
irr), upper critical fields (
H
c2) and coherence lengths at 0
K (
ξ(0)) were calculated from the resistivity versus temperature (
R–
T) curves under DC magnetic fields up to 7
T. The superconducting transition temperature,
T
c, and activation energy,
U
0, were found to decrease with increase in Gd concentration and with increase in applied magnetic field. The offset transition temperature of the pure (Gd00) sample without applied magnetic field is 108
K, whereas for Gd05 sample, the offset transition temperature drops to 5
K with 7
T applied magnetic field. The activation energy of the Gd00 sample without applied magnetic field is 34,980
K, and for Gd05 sample with 7
T applied field it is 98
K.
H
irr and
H
c2 values also decrease with increase in Gd addition. The possible reasons for the observed degradation in microstructural and superconducting properties due to Gd addition were discussed.</abstract><cop>Kidlington</cop><pub>Elsevier B.V</pub><doi>10.1016/j.physb.2010.12.008</doi><tpages>5</tpages></addata></record> |
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subjects | ACTIVATION ENERGY BSCCO-2223 Condensed matter Condensed matter: electronic structure, electrical, magnetic, and optical properties Effects of crystal defects, doping and substitution ELECTRICAL CONDUCTIVITY Electrical resistivity Exact sciences and technology High temperature superconductors MAGNETIC FIELD Magnetic fields MATHEMATICAL ANALYSIS Mixed state, critical fields, and surface sheath Offsets Physics Properties of type I and type II superconductors Rare earth addition SUPERCONDUCTIVITY SUPERCONDUCTORS TRANSITION TEMPERATURE Transition temperature variations |
title | Effect of Gd addition on the activation energies of Bi-2223 superconductor |
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