Modulated structure and superconductivity in 2D electron-hole lattice system
Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing...
Ausführliche Beschreibung
Autor*in: |
Kuwata, S. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
1994 |
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Anmerkung: |
© Plenum Publishing Corporation 1994 |
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Übergeordnetes Werk: |
Enthalten in: Journal of superconductivity - Kluwer Academic Publishers-Plenum Publishers, 1988, 7(1994), 4 vom: Aug., Seite 777-781 |
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Übergeordnetes Werk: |
volume:7 ; year:1994 ; number:4 ; month:08 ; pages:777-781 |
Links: |
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DOI / URN: |
10.1007/BF00721663 |
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Katalog-ID: |
OLC2057263487 |
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10.1007/BF00721663 doi (DE-627)OLC2057263487 (DE-He213)BF00721663-p DE-627 ger DE-627 rakwb eng 530 VZ Kuwata, S. verfasserin aut Modulated structure and superconductivity in 2D electron-hole lattice system 1994 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. Kinase, W. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 7(1994), 4 vom: Aug., Seite 777-781 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:7 year:1994 number:4 month:08 pages:777-781 https://doi.org/10.1007/BF00721663 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 AR 7 1994 4 08 777-781 |
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10.1007/BF00721663 doi (DE-627)OLC2057263487 (DE-He213)BF00721663-p DE-627 ger DE-627 rakwb eng 530 VZ Kuwata, S. verfasserin aut Modulated structure and superconductivity in 2D electron-hole lattice system 1994 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. Kinase, W. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 7(1994), 4 vom: Aug., Seite 777-781 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:7 year:1994 number:4 month:08 pages:777-781 https://doi.org/10.1007/BF00721663 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 AR 7 1994 4 08 777-781 |
allfields_unstemmed |
10.1007/BF00721663 doi (DE-627)OLC2057263487 (DE-He213)BF00721663-p DE-627 ger DE-627 rakwb eng 530 VZ Kuwata, S. verfasserin aut Modulated structure and superconductivity in 2D electron-hole lattice system 1994 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. Kinase, W. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 7(1994), 4 vom: Aug., Seite 777-781 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:7 year:1994 number:4 month:08 pages:777-781 https://doi.org/10.1007/BF00721663 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 AR 7 1994 4 08 777-781 |
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10.1007/BF00721663 doi (DE-627)OLC2057263487 (DE-He213)BF00721663-p DE-627 ger DE-627 rakwb eng 530 VZ Kuwata, S. verfasserin aut Modulated structure and superconductivity in 2D electron-hole lattice system 1994 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. Kinase, W. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 7(1994), 4 vom: Aug., Seite 777-781 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:7 year:1994 number:4 month:08 pages:777-781 https://doi.org/10.1007/BF00721663 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 AR 7 1994 4 08 777-781 |
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Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. © Plenum Publishing Corporation 1994 |
abstractGer |
Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. © Plenum Publishing Corporation 1994 |
abstract_unstemmed |
Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. © Plenum Publishing Corporation 1994 |
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The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kinase, W.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of superconductivity</subfield><subfield code="d">Kluwer Academic Publishers-Plenum Publishers, 1988</subfield><subfield code="g">7(1994), 4 vom: Aug., Seite 777-781</subfield><subfield code="w">(DE-627)130413186</subfield><subfield code="w">(DE-600)623132-9</subfield><subfield code="w">(DE-576)01866539X</subfield><subfield code="x">0896-1107</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:7</subfield><subfield code="g">year:1994</subfield><subfield code="g">number:4</subfield><subfield code="g">month:08</subfield><subfield code="g">pages:777-781</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF00721663</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-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4036</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4318</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">7</subfield><subfield code="j">1994</subfield><subfield code="e">4</subfield><subfield code="c">08</subfield><subfield code="h">777-781</subfield></datafield></record></collection>
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