Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $
Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The e...
Ausführliche Beschreibung
Autor*in: |
Vijayashree, V [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
1991 |
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Schlagwörter: |
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Anmerkung: |
© Indian Academy of Sciences 1991 |
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Übergeordnetes Werk: |
Enthalten in: Bulletin of materials science - Springer India, 1979, 14(1991), 3 vom: Juni, Seite 827-830 |
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Übergeordnetes Werk: |
volume:14 ; year:1991 ; number:3 ; month:06 ; pages:827-830 |
Links: |
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DOI / URN: |
10.1007/BF02744734 |
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Katalog-ID: |
OLC2055181637 |
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10.1007/BF02744734 doi (DE-627)OLC2055181637 (DE-He213)BF02744734-p DE-627 ger DE-627 rakwb eng 600 VZ Vijayashree, V verfasserin aut Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $ 1991 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1991 Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model. Thermopower linear variation exponential enhancement two-band model Subramaniam, C K aut Srinivasan, R aut Gopalakrishnan, I K aut Sastry, PVPSS aut Yakhmi, J V aut Iyer, R M aut Enthalten in Bulletin of materials science Springer India, 1979 14(1991), 3 vom: Juni, Seite 827-830 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:14 year:1991 number:3 month:06 pages:827-830 https://doi.org/10.1007/BF02744734 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 AR 14 1991 3 06 827-830 |
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10.1007/BF02744734 doi (DE-627)OLC2055181637 (DE-He213)BF02744734-p DE-627 ger DE-627 rakwb eng 600 VZ Vijayashree, V verfasserin aut Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $ 1991 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1991 Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model. Thermopower linear variation exponential enhancement two-band model Subramaniam, C K aut Srinivasan, R aut Gopalakrishnan, I K aut Sastry, PVPSS aut Yakhmi, J V aut Iyer, R M aut Enthalten in Bulletin of materials science Springer India, 1979 14(1991), 3 vom: Juni, Seite 827-830 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:14 year:1991 number:3 month:06 pages:827-830 https://doi.org/10.1007/BF02744734 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 AR 14 1991 3 06 827-830 |
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10.1007/BF02744734 doi (DE-627)OLC2055181637 (DE-He213)BF02744734-p DE-627 ger DE-627 rakwb eng 600 VZ Vijayashree, V verfasserin aut Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $ 1991 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1991 Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model. Thermopower linear variation exponential enhancement two-band model Subramaniam, C K aut Srinivasan, R aut Gopalakrishnan, I K aut Sastry, PVPSS aut Yakhmi, J V aut Iyer, R M aut Enthalten in Bulletin of materials science Springer India, 1979 14(1991), 3 vom: Juni, Seite 827-830 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:14 year:1991 number:3 month:06 pages:827-830 https://doi.org/10.1007/BF02744734 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 AR 14 1991 3 06 827-830 |
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10.1007/BF02744734 doi (DE-627)OLC2055181637 (DE-He213)BF02744734-p DE-627 ger DE-627 rakwb eng 600 VZ Vijayashree, V verfasserin aut Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $ 1991 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1991 Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model. Thermopower linear variation exponential enhancement two-band model Subramaniam, C K aut Srinivasan, R aut Gopalakrishnan, I K aut Sastry, PVPSS aut Yakhmi, J V aut Iyer, R M aut Enthalten in Bulletin of materials science Springer India, 1979 14(1991), 3 vom: Juni, Seite 827-830 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:14 year:1991 number:3 month:06 pages:827-830 https://doi.org/10.1007/BF02744734 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 AR 14 1991 3 06 827-830 |
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10.1007/BF02744734 doi (DE-627)OLC2055181637 (DE-He213)BF02744734-p DE-627 ger DE-627 rakwb eng 600 VZ Vijayashree, V verfasserin aut Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $ 1991 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1991 Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model. Thermopower linear variation exponential enhancement two-band model Subramaniam, C K aut Srinivasan, R aut Gopalakrishnan, I K aut Sastry, PVPSS aut Yakhmi, J V aut Iyer, R M aut Enthalten in Bulletin of materials science Springer India, 1979 14(1991), 3 vom: Juni, Seite 827-830 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:14 year:1991 number:3 month:06 pages:827-830 https://doi.org/10.1007/BF02744734 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 AR 14 1991 3 06 827-830 |
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Vijayashree, V |
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600 VZ Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $ Thermopower linear variation exponential enhancement two-band model |
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Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $ |
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thermoelectric power of single-phase samples of $ tl_{2} $$ caba_{2} $$ cu_{2} $$ o_{y} $ and $ ba_{2} $$ casr_{2} $$ cu_{2} $$ o_{y} $ |
title_auth |
Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $ |
abstract |
Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model. © Indian Academy of Sciences 1991 |
abstractGer |
Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model. © Indian Academy of Sciences 1991 |
abstract_unstemmed |
Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model. © Indian Academy of Sciences 1991 |
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Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $ |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2055181637</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230402060719.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s1991 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02744734</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2055181637</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF02744734-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">600</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Vijayashree, V</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Thermoelectric power of single-phase samples of $ Tl_{2} $$ CaBa_{2} $$ Cu_{2} $$ O_{y} $ and $ Ba_{2} $$ CaSr_{2} $$ Cu_{2} $$ O_{y} $</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1991</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Indian Academy of Sciences 1991</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-Tc. The thermopower was positive and decreased linearly with increasing temperature aboveTc (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Thermopower</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">linear variation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">exponential enhancement</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">two-band model</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Subramaniam, C K</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Srinivasan, R</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Gopalakrishnan, I K</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Sastry, PVPSS</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Yakhmi, J V</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Iyer, R M</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Bulletin of materials science</subfield><subfield code="d">Springer India, 1979</subfield><subfield code="g">14(1991), 3 vom: Juni, Seite 827-830</subfield><subfield code="w">(DE-627)130547476</subfield><subfield code="w">(DE-600)781668-6</subfield><subfield code="w">(DE-576)9130547474</subfield><subfield code="x">0250-4707</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:14</subfield><subfield code="g">year:1991</subfield><subfield code="g">number:3</subfield><subfield code="g">month:06</subfield><subfield code="g">pages:827-830</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF02744734</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_30</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">14</subfield><subfield code="j">1991</subfield><subfield code="e">3</subfield><subfield code="c">06</subfield><subfield code="h">827-830</subfield></datafield></record></collection>
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