Electronic Structure of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $ Revealed by Angle-Resolved Photoemission Spectroscopy
Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital de...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Mizokawa, T. [verfasserIn] Sudayama, T. [verfasserIn] Wakisaka, Y. [verfasserIn] Morinaga, R. [verfasserIn] Sato, T. J. [verfasserIn] Arita, M. [verfasserIn] Namatame, H. [verfasserIn] Taniguchi, M. [verfasserIn] Saini, N. L. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2010 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Journal of superconductivity - Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988, 24(2010), 3 vom: 30. Dez., Seite 1133-1136 |
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| Übergeordnetes Werk: |
volume:24 ; year:2010 ; number:3 ; day:30 ; month:12 ; pages:1133-1136 |
| Links: |
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| DOI / URN: |
10.1007/s10948-010-1095-z |
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SPR014872366 |
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| 520 | |a Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital degeneracy is expected. This observation suggests that the Jahn–Teller type instability is playing an important role in the tetragonal phase above Ts. Below Ts, the spectral weight of 0–100 meV is reconstructed to form flat bands at 70–100 meV and Fermi surfaces, consistent with the orbital-dependent excitonic coupling. In the optimally doped and overdoped regimes, the hole pocket around the Γ point and the electron pocket around the M point are apparently nested, indicating that the doping dependence of the superconducting transition temperature cannot be explained by the nesting scenario and that the unusual electron–lattice fluctuation due to the orbital degeneracy is important. | ||
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| 700 | 1 | |a Sudayama, T. |e verfasserin |4 aut | |
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| 700 | 1 | |a Sato, T. J. |e verfasserin |4 aut | |
| 700 | 1 | |a Arita, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Namatame, H. |e verfasserin |4 aut | |
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10.1007/s10948-010-1095-z doi (DE-627)SPR014872366 (SPR)s10948-010-1095-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Mizokawa, T. verfasserin aut Electronic Structure of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $ Revealed by Angle-Resolved Photoemission Spectroscopy 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital degeneracy is expected. This observation suggests that the Jahn–Teller type instability is playing an important role in the tetragonal phase above Ts. Below Ts, the spectral weight of 0–100 meV is reconstructed to form flat bands at 70–100 meV and Fermi surfaces, consistent with the orbital-dependent excitonic coupling. In the optimally doped and overdoped regimes, the hole pocket around the Γ point and the electron pocket around the M point are apparently nested, indicating that the doping dependence of the superconducting transition temperature cannot be explained by the nesting scenario and that the unusual electron–lattice fluctuation due to the orbital degeneracy is important. ARPES (dpeaa)DE-He213 FeAs layer (dpeaa)DE-He213 Orbital degeneracy (dpeaa)DE-He213 Excitonic insulator (dpeaa)DE-He213 Sudayama, T. verfasserin aut Wakisaka, Y. verfasserin aut Morinaga, R. verfasserin aut Sato, T. J. verfasserin aut Arita, M. verfasserin aut Namatame, H. verfasserin aut Taniguchi, M. verfasserin aut Saini, N. L. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 24(2010), 3 vom: 30. Dez., Seite 1133-1136 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:24 year:2010 number:3 day:30 month:12 pages:1133-1136 https://dx.doi.org/10.1007/s10948-010-1095-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 24 2010 3 30 12 1133-1136 |
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10.1007/s10948-010-1095-z doi (DE-627)SPR014872366 (SPR)s10948-010-1095-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Mizokawa, T. verfasserin aut Electronic Structure of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $ Revealed by Angle-Resolved Photoemission Spectroscopy 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital degeneracy is expected. This observation suggests that the Jahn–Teller type instability is playing an important role in the tetragonal phase above Ts. Below Ts, the spectral weight of 0–100 meV is reconstructed to form flat bands at 70–100 meV and Fermi surfaces, consistent with the orbital-dependent excitonic coupling. In the optimally doped and overdoped regimes, the hole pocket around the Γ point and the electron pocket around the M point are apparently nested, indicating that the doping dependence of the superconducting transition temperature cannot be explained by the nesting scenario and that the unusual electron–lattice fluctuation due to the orbital degeneracy is important. ARPES (dpeaa)DE-He213 FeAs layer (dpeaa)DE-He213 Orbital degeneracy (dpeaa)DE-He213 Excitonic insulator (dpeaa)DE-He213 Sudayama, T. verfasserin aut Wakisaka, Y. verfasserin aut Morinaga, R. verfasserin aut Sato, T. J. verfasserin aut Arita, M. verfasserin aut Namatame, H. verfasserin aut Taniguchi, M. verfasserin aut Saini, N. L. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 24(2010), 3 vom: 30. Dez., Seite 1133-1136 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:24 year:2010 number:3 day:30 month:12 pages:1133-1136 https://dx.doi.org/10.1007/s10948-010-1095-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 24 2010 3 30 12 1133-1136 |
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10.1007/s10948-010-1095-z doi (DE-627)SPR014872366 (SPR)s10948-010-1095-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Mizokawa, T. verfasserin aut Electronic Structure of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $ Revealed by Angle-Resolved Photoemission Spectroscopy 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital degeneracy is expected. This observation suggests that the Jahn–Teller type instability is playing an important role in the tetragonal phase above Ts. Below Ts, the spectral weight of 0–100 meV is reconstructed to form flat bands at 70–100 meV and Fermi surfaces, consistent with the orbital-dependent excitonic coupling. In the optimally doped and overdoped regimes, the hole pocket around the Γ point and the electron pocket around the M point are apparently nested, indicating that the doping dependence of the superconducting transition temperature cannot be explained by the nesting scenario and that the unusual electron–lattice fluctuation due to the orbital degeneracy is important. ARPES (dpeaa)DE-He213 FeAs layer (dpeaa)DE-He213 Orbital degeneracy (dpeaa)DE-He213 Excitonic insulator (dpeaa)DE-He213 Sudayama, T. verfasserin aut Wakisaka, Y. verfasserin aut Morinaga, R. verfasserin aut Sato, T. J. verfasserin aut Arita, M. verfasserin aut Namatame, H. verfasserin aut Taniguchi, M. verfasserin aut Saini, N. L. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 24(2010), 3 vom: 30. Dez., Seite 1133-1136 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:24 year:2010 number:3 day:30 month:12 pages:1133-1136 https://dx.doi.org/10.1007/s10948-010-1095-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 24 2010 3 30 12 1133-1136 |
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10.1007/s10948-010-1095-z doi (DE-627)SPR014872366 (SPR)s10948-010-1095-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Mizokawa, T. verfasserin aut Electronic Structure of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $ Revealed by Angle-Resolved Photoemission Spectroscopy 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital degeneracy is expected. This observation suggests that the Jahn–Teller type instability is playing an important role in the tetragonal phase above Ts. Below Ts, the spectral weight of 0–100 meV is reconstructed to form flat bands at 70–100 meV and Fermi surfaces, consistent with the orbital-dependent excitonic coupling. In the optimally doped and overdoped regimes, the hole pocket around the Γ point and the electron pocket around the M point are apparently nested, indicating that the doping dependence of the superconducting transition temperature cannot be explained by the nesting scenario and that the unusual electron–lattice fluctuation due to the orbital degeneracy is important. ARPES (dpeaa)DE-He213 FeAs layer (dpeaa)DE-He213 Orbital degeneracy (dpeaa)DE-He213 Excitonic insulator (dpeaa)DE-He213 Sudayama, T. verfasserin aut Wakisaka, Y. verfasserin aut Morinaga, R. verfasserin aut Sato, T. J. verfasserin aut Arita, M. verfasserin aut Namatame, H. verfasserin aut Taniguchi, M. verfasserin aut Saini, N. L. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 24(2010), 3 vom: 30. Dez., Seite 1133-1136 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:24 year:2010 number:3 day:30 month:12 pages:1133-1136 https://dx.doi.org/10.1007/s10948-010-1095-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 24 2010 3 30 12 1133-1136 |
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10.1007/s10948-010-1095-z doi (DE-627)SPR014872366 (SPR)s10948-010-1095-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Mizokawa, T. verfasserin aut Electronic Structure of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $ Revealed by Angle-Resolved Photoemission Spectroscopy 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital degeneracy is expected. This observation suggests that the Jahn–Teller type instability is playing an important role in the tetragonal phase above Ts. Below Ts, the spectral weight of 0–100 meV is reconstructed to form flat bands at 70–100 meV and Fermi surfaces, consistent with the orbital-dependent excitonic coupling. In the optimally doped and overdoped regimes, the hole pocket around the Γ point and the electron pocket around the M point are apparently nested, indicating that the doping dependence of the superconducting transition temperature cannot be explained by the nesting scenario and that the unusual electron–lattice fluctuation due to the orbital degeneracy is important. ARPES (dpeaa)DE-He213 FeAs layer (dpeaa)DE-He213 Orbital degeneracy (dpeaa)DE-He213 Excitonic insulator (dpeaa)DE-He213 Sudayama, T. verfasserin aut Wakisaka, Y. verfasserin aut Morinaga, R. verfasserin aut Sato, T. J. verfasserin aut Arita, M. verfasserin aut Namatame, H. verfasserin aut Taniguchi, M. verfasserin aut Saini, N. L. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 24(2010), 3 vom: 30. Dez., Seite 1133-1136 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:24 year:2010 number:3 day:30 month:12 pages:1133-1136 https://dx.doi.org/10.1007/s10948-010-1095-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 24 2010 3 30 12 1133-1136 |
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Mizokawa, T. @@aut@@ Sudayama, T. @@aut@@ Wakisaka, Y. @@aut@@ Morinaga, R. @@aut@@ Sato, T. J. @@aut@@ Arita, M. @@aut@@ Namatame, H. @@aut@@ Taniguchi, M. @@aut@@ Saini, N. L. @@aut@@ |
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Electronic Structure of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $ Revealed by Angle-Resolved Photoemission Spectroscopy |
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electronic structure of $ bafe_{2−x} %$ co_{x} %$ as_{2} $ revealed by angle-resolved photoemission spectroscopy |
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Electronic Structure of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $ Revealed by Angle-Resolved Photoemission Spectroscopy |
| abstract |
Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital degeneracy is expected. This observation suggests that the Jahn–Teller type instability is playing an important role in the tetragonal phase above Ts. Below Ts, the spectral weight of 0–100 meV is reconstructed to form flat bands at 70–100 meV and Fermi surfaces, consistent with the orbital-dependent excitonic coupling. In the optimally doped and overdoped regimes, the hole pocket around the Γ point and the electron pocket around the M point are apparently nested, indicating that the doping dependence of the superconducting transition temperature cannot be explained by the nesting scenario and that the unusual electron–lattice fluctuation due to the orbital degeneracy is important. |
| abstractGer |
Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital degeneracy is expected. This observation suggests that the Jahn–Teller type instability is playing an important role in the tetragonal phase above Ts. Below Ts, the spectral weight of 0–100 meV is reconstructed to form flat bands at 70–100 meV and Fermi surfaces, consistent with the orbital-dependent excitonic coupling. In the optimally doped and overdoped regimes, the hole pocket around the Γ point and the electron pocket around the M point are apparently nested, indicating that the doping dependence of the superconducting transition temperature cannot be explained by the nesting scenario and that the unusual electron–lattice fluctuation due to the orbital degeneracy is important. |
| abstract_unstemmed |
Abstract We report an angle-resolved photoemission spectroscopy study of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $. For x=0, above the structural and magnetic transition temperature (Ts), the spectral weight near the Fermi level is considerably suppressed around the Γ point where the Fe 3d yz/zx orbital degeneracy is expected. This observation suggests that the Jahn–Teller type instability is playing an important role in the tetragonal phase above Ts. Below Ts, the spectral weight of 0–100 meV is reconstructed to form flat bands at 70–100 meV and Fermi surfaces, consistent with the orbital-dependent excitonic coupling. In the optimally doped and overdoped regimes, the hole pocket around the Γ point and the electron pocket around the M point are apparently nested, indicating that the doping dependence of the superconducting transition temperature cannot be explained by the nesting scenario and that the unusual electron–lattice fluctuation due to the orbital degeneracy is important. |
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Electronic Structure of $ BaFe_{2−x} %$ Co_{x} %$ As_{2} $ Revealed by Angle-Resolved Photoemission Spectroscopy |
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