On electronic current in NiO
Conduction by the movement of an extra electron which is tightly bound ro an ion in an ionic lattice is discussed. We assume that the wave function of the electron is localized closely around an ion and the motion of the electron is so slow that lattice polarization is induced around the electron. I...
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| Autor*in: |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1958 |
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| Reproduktion: |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
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| Übergeordnetes Werk: |
in: Journal of Physics and Chemistry of Solids - Amsterdam : Elsevier, 5(1958), 1-2, Seite 34-43 |
| Übergeordnetes Werk: |
volume:5 ; year:1958 ; number:1-2 ; pages:34-43 |
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| 520 | |a Conduction by the movement of an extra electron which is tightly bound ro an ion in an ionic lattice is discussed. We assume that the wave function of the electron is localized closely around an ion and the motion of the electron is so slow that lattice polarization is induced around the electron. In this case the conduction mechanism may not be explained by the usual band theory, but it may be better to use a Heitler-London picture and to interpret the current as a result of wandering of the electron from ion to ion. We use this conduction mechanism to explain the electronic current which appears in NiO and LaMnO"3 crystals. | ||
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(DE-627)NLEJ17824175X (DE-599)GBVNLZ17824175X DE-627 ger DE-627 rakwb eng On electronic current in NiO 1958 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Conduction by the movement of an extra electron which is tightly bound ro an ion in an ionic lattice is discussed. We assume that the wave function of the electron is localized closely around an ion and the motion of the electron is so slow that lattice polarization is induced around the electron. In this case the conduction mechanism may not be explained by the usual band theory, but it may be better to use a Heitler-London picture and to interpret the current as a result of wandering of the electron from ion to ion. We use this conduction mechanism to explain the electronic current which appears in NiO and LaMnO"3 crystals. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Yamashita, J. oth Kurosawa, T. oth in Journal of Physics and Chemistry of Solids Amsterdam : Elsevier 5(1958), 1-2, Seite 34-43 (DE-627)NLEJ177273895 (DE-600)1491914-X 0022-3697 nnns volume:5 year:1958 number:1-2 pages:34-43 http://linkinghub.elsevier.com/retrieve/pii/0022-3697(58)90129-X GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 5 1958 1-2 34-43 |
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(DE-627)NLEJ17824175X (DE-599)GBVNLZ17824175X DE-627 ger DE-627 rakwb eng On electronic current in NiO 1958 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Conduction by the movement of an extra electron which is tightly bound ro an ion in an ionic lattice is discussed. We assume that the wave function of the electron is localized closely around an ion and the motion of the electron is so slow that lattice polarization is induced around the electron. In this case the conduction mechanism may not be explained by the usual band theory, but it may be better to use a Heitler-London picture and to interpret the current as a result of wandering of the electron from ion to ion. We use this conduction mechanism to explain the electronic current which appears in NiO and LaMnO"3 crystals. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Yamashita, J. oth Kurosawa, T. oth in Journal of Physics and Chemistry of Solids Amsterdam : Elsevier 5(1958), 1-2, Seite 34-43 (DE-627)NLEJ177273895 (DE-600)1491914-X 0022-3697 nnns volume:5 year:1958 number:1-2 pages:34-43 http://linkinghub.elsevier.com/retrieve/pii/0022-3697(58)90129-X GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 5 1958 1-2 34-43 |
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(DE-627)NLEJ17824175X (DE-599)GBVNLZ17824175X DE-627 ger DE-627 rakwb eng On electronic current in NiO 1958 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Conduction by the movement of an extra electron which is tightly bound ro an ion in an ionic lattice is discussed. We assume that the wave function of the electron is localized closely around an ion and the motion of the electron is so slow that lattice polarization is induced around the electron. In this case the conduction mechanism may not be explained by the usual band theory, but it may be better to use a Heitler-London picture and to interpret the current as a result of wandering of the electron from ion to ion. We use this conduction mechanism to explain the electronic current which appears in NiO and LaMnO"3 crystals. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Yamashita, J. oth Kurosawa, T. oth in Journal of Physics and Chemistry of Solids Amsterdam : Elsevier 5(1958), 1-2, Seite 34-43 (DE-627)NLEJ177273895 (DE-600)1491914-X 0022-3697 nnns volume:5 year:1958 number:1-2 pages:34-43 http://linkinghub.elsevier.com/retrieve/pii/0022-3697(58)90129-X GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 5 1958 1-2 34-43 |
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(DE-627)NLEJ17824175X (DE-599)GBVNLZ17824175X DE-627 ger DE-627 rakwb eng On electronic current in NiO 1958 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Conduction by the movement of an extra electron which is tightly bound ro an ion in an ionic lattice is discussed. We assume that the wave function of the electron is localized closely around an ion and the motion of the electron is so slow that lattice polarization is induced around the electron. In this case the conduction mechanism may not be explained by the usual band theory, but it may be better to use a Heitler-London picture and to interpret the current as a result of wandering of the electron from ion to ion. We use this conduction mechanism to explain the electronic current which appears in NiO and LaMnO"3 crystals. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Yamashita, J. oth Kurosawa, T. oth in Journal of Physics and Chemistry of Solids Amsterdam : Elsevier 5(1958), 1-2, Seite 34-43 (DE-627)NLEJ177273895 (DE-600)1491914-X 0022-3697 nnns volume:5 year:1958 number:1-2 pages:34-43 http://linkinghub.elsevier.com/retrieve/pii/0022-3697(58)90129-X GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 5 1958 1-2 34-43 |
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Conduction by the movement of an extra electron which is tightly bound ro an ion in an ionic lattice is discussed. We assume that the wave function of the electron is localized closely around an ion and the motion of the electron is so slow that lattice polarization is induced around the electron. In this case the conduction mechanism may not be explained by the usual band theory, but it may be better to use a Heitler-London picture and to interpret the current as a result of wandering of the electron from ion to ion. We use this conduction mechanism to explain the electronic current which appears in NiO and LaMnO"3 crystals. |
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Conduction by the movement of an extra electron which is tightly bound ro an ion in an ionic lattice is discussed. We assume that the wave function of the electron is localized closely around an ion and the motion of the electron is so slow that lattice polarization is induced around the electron. In this case the conduction mechanism may not be explained by the usual band theory, but it may be better to use a Heitler-London picture and to interpret the current as a result of wandering of the electron from ion to ion. We use this conduction mechanism to explain the electronic current which appears in NiO and LaMnO"3 crystals. |
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Conduction by the movement of an extra electron which is tightly bound ro an ion in an ionic lattice is discussed. We assume that the wave function of the electron is localized closely around an ion and the motion of the electron is so slow that lattice polarization is induced around the electron. In this case the conduction mechanism may not be explained by the usual band theory, but it may be better to use a Heitler-London picture and to interpret the current as a result of wandering of the electron from ion to ion. We use this conduction mechanism to explain the electronic current which appears in NiO and LaMnO"3 crystals. |
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