Pseudogap in the Normal State of Cuprates
Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of s...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Bouvier, J. [verfasserIn] |
|---|
| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2000 |
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| Anmerkung: |
© Plenum Publishing Corporation 2000 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of superconductivity - Kluwer Academic Publishers-Plenum Publishers, 1988, 13(2000), 6 vom: Dez., Seite 995-998 |
|---|---|
| Übergeordnetes Werk: |
volume:13 ; year:2000 ; number:6 ; month:12 ; pages:995-998 |
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| DOI / URN: |
10.1023/A:1026414627525 |
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| 520 | |a Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of state (DOS) near the Fermi level (FL). We show that this model explains most of the observed features of the so-called pseudogap in the normal state and in particular its value, anisotropy, and variation with doping. | ||
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10.1023/A:1026414627525 doi (DE-627)OLC2057272176 (DE-He213)A:1026414627525-p DE-627 ger DE-627 rakwb eng 530 VZ Bouvier, J. verfasserin aut Pseudogap in the Normal State of Cuprates 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 2000 Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of state (DOS) near the Fermi level (FL). We show that this model explains most of the observed features of the so-called pseudogap in the normal state and in particular its value, anisotropy, and variation with doping. Bok, J. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 13(2000), 6 vom: Dez., Seite 995-998 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:13 year:2000 number:6 month:12 pages:995-998 https://doi.org/10.1023/A:1026414627525 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_31 GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 AR 13 2000 6 12 995-998 |
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10.1023/A:1026414627525 doi (DE-627)OLC2057272176 (DE-He213)A:1026414627525-p DE-627 ger DE-627 rakwb eng 530 VZ Bouvier, J. verfasserin aut Pseudogap in the Normal State of Cuprates 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 2000 Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of state (DOS) near the Fermi level (FL). We show that this model explains most of the observed features of the so-called pseudogap in the normal state and in particular its value, anisotropy, and variation with doping. Bok, J. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 13(2000), 6 vom: Dez., Seite 995-998 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:13 year:2000 number:6 month:12 pages:995-998 https://doi.org/10.1023/A:1026414627525 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_31 GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 AR 13 2000 6 12 995-998 |
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10.1023/A:1026414627525 doi (DE-627)OLC2057272176 (DE-He213)A:1026414627525-p DE-627 ger DE-627 rakwb eng 530 VZ Bouvier, J. verfasserin aut Pseudogap in the Normal State of Cuprates 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 2000 Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of state (DOS) near the Fermi level (FL). We show that this model explains most of the observed features of the so-called pseudogap in the normal state and in particular its value, anisotropy, and variation with doping. Bok, J. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 13(2000), 6 vom: Dez., Seite 995-998 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:13 year:2000 number:6 month:12 pages:995-998 https://doi.org/10.1023/A:1026414627525 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_31 GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 AR 13 2000 6 12 995-998 |
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10.1023/A:1026414627525 doi (DE-627)OLC2057272176 (DE-He213)A:1026414627525-p DE-627 ger DE-627 rakwb eng 530 VZ Bouvier, J. verfasserin aut Pseudogap in the Normal State of Cuprates 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 2000 Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of state (DOS) near the Fermi level (FL). We show that this model explains most of the observed features of the so-called pseudogap in the normal state and in particular its value, anisotropy, and variation with doping. Bok, J. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 13(2000), 6 vom: Dez., Seite 995-998 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:13 year:2000 number:6 month:12 pages:995-998 https://doi.org/10.1023/A:1026414627525 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_31 GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 AR 13 2000 6 12 995-998 |
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Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of state (DOS) near the Fermi level (FL). We show that this model explains most of the observed features of the so-called pseudogap in the normal state and in particular its value, anisotropy, and variation with doping. © Plenum Publishing Corporation 2000 |
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Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of state (DOS) near the Fermi level (FL). We show that this model explains most of the observed features of the so-called pseudogap in the normal state and in particular its value, anisotropy, and variation with doping. © Plenum Publishing Corporation 2000 |
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Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of state (DOS) near the Fermi level (FL). We show that this model explains most of the observed features of the so-called pseudogap in the normal state and in particular its value, anisotropy, and variation with doping. © Plenum Publishing Corporation 2000 |
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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">OLC2057272176</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503152756.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s2000 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1023/A:1026414627525</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2057272176</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)A:1026414627525-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">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Bouvier, J.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Pseudogap in the Normal State of Cuprates</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2000</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">© Plenum Publishing Corporation 2000</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract We consider underdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as $ 10^{−5} $ $ m^{2} $ $ s^{−1} $. In these conditions, Coulomb interaction between electrons must be taken into account. The main effect is to open a dip and even a gap in the density of state (DOS) near the Fermi level (FL). We show that this model explains most of the observed features of the so-called pseudogap in the normal state and in particular its value, anisotropy, and variation with doping.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Bok, J.</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">13(2000), 6 vom: Dez., Seite 995-998</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:13</subfield><subfield code="g">year:2000</subfield><subfield code="g">number:6</subfield><subfield code="g">month:12</subfield><subfield code="g">pages:995-998</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1023/A:1026414627525</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_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</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="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">13</subfield><subfield code="j">2000</subfield><subfield code="e">6</subfield><subfield code="c">12</subfield><subfield code="h">995-998</subfield></datafield></record></collection>
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