Electronic structure of La1-xSrxMnO3 studied by photoemission and x-ray-absorption spectroscopy

T. Saitoh, A. E. Bocquet, Takashi Mizokawa, H. Namatame, A. Fujimori, M. Abbate, Y. Takeda, M. Takano

研究成果: Article

494 引用 (Scopus)

抄録

The electronic structure of La1-xSrxMnO3 has been studied by photoemission and O 1s x-ray-absorption spectroscopy. Spectra of the Mn 2p core levels and the valence bands for LaMnO3 and SrMnO3 have been analyzed using a configuration-interaction cluster model. The ground state of LaMnO3 is found to be mixed d4 and d5L states and that of SrMnO3 to be heavily mixed d3 and d4L states, reflecting their strong covalency. The character of the band gap of LaMnO3 is of the p-to-d charge-transfer type while that of SrMnO3 has considerable p-p character as well as p-d character. Holes doped into LaMnO3 mainly of oxygen p character are coupled antiferromagnetically with the d4 local moments of the Mn3+ ions and become itinerant, thus aligning the Mn moments ferromagnetically. The changes in the electronic structure with carrier doping are not of the rigid band type: By La substitution for SrMnO3, the so-called in-gap spectral weight (of eg symmetry) appears with its peak located 1-2 eV below the Fermi level and grows in intensity with increasing La concentration, while the spectral intensity of the eg states above the Fermi level decreases, showing a transfer of spectral weight from the unoccupied to the occupied eg states with electron doping. Meanwhile, the intensity at the Fermi level remains low even in the metallic phase (0.2x0.6). The energy shifts of core-level peaks and valence-band features with x suggest a downward shift of the Fermi level with hole doping, but the shift is found to be very small in the metallic phase. The importance of the orbital degeneracy of the eg band and possible orbital fluctuations in the ferromagnetic phase are pointed out.

元の言語English
ページ(範囲)13942-13951
ページ数10
ジャーナルPhysical Review B
51
発行部数20
DOI
出版物ステータスPublished - 1995
外部発表Yes

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Photoemission
Fermi level
Absorption spectroscopy
x ray absorption
x ray spectroscopy
Electronic structure
absorption spectroscopy
photoelectric emission
electronic structure
X rays
Core levels
Doping (additives)
Valence bands
shift
Ground state
valence
moments
Charge transfer
orbitals
Energy gap

ASJC Scopus subject areas

  • Condensed Matter Physics

これを引用

Saitoh, T., Bocquet, A. E., Mizokawa, T., Namatame, H., Fujimori, A., Abbate, M., ... Takano, M. (1995). Electronic structure of La1-xSrxMnO3 studied by photoemission and x-ray-absorption spectroscopy. Physical Review B, 51(20), 13942-13951. https://doi.org/10.1103/PhysRevB.51.13942

Electronic structure of La1-xSrxMnO3 studied by photoemission and x-ray-absorption spectroscopy. / Saitoh, T.; Bocquet, A. E.; Mizokawa, Takashi; Namatame, H.; Fujimori, A.; Abbate, M.; Takeda, Y.; Takano, M.

:: Physical Review B, 巻 51, 番号 20, 1995, p. 13942-13951.

研究成果: Article

Saitoh, T, Bocquet, AE, Mizokawa, T, Namatame, H, Fujimori, A, Abbate, M, Takeda, Y & Takano, M 1995, 'Electronic structure of La1-xSrxMnO3 studied by photoemission and x-ray-absorption spectroscopy', Physical Review B, 巻. 51, 番号 20, pp. 13942-13951. https://doi.org/10.1103/PhysRevB.51.13942
Saitoh, T. ; Bocquet, A. E. ; Mizokawa, Takashi ; Namatame, H. ; Fujimori, A. ; Abbate, M. ; Takeda, Y. ; Takano, M. / Electronic structure of La1-xSrxMnO3 studied by photoemission and x-ray-absorption spectroscopy. :: Physical Review B. 1995 ; 巻 51, 番号 20. pp. 13942-13951.
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abstract = "The electronic structure of La1-xSrxMnO3 has been studied by photoemission and O 1s x-ray-absorption spectroscopy. Spectra of the Mn 2p core levels and the valence bands for LaMnO3 and SrMnO3 have been analyzed using a configuration-interaction cluster model. The ground state of LaMnO3 is found to be mixed d4 and d5L states and that of SrMnO3 to be heavily mixed d3 and d4L states, reflecting their strong covalency. The character of the band gap of LaMnO3 is of the p-to-d charge-transfer type while that of SrMnO3 has considerable p-p character as well as p-d character. Holes doped into LaMnO3 mainly of oxygen p character are coupled antiferromagnetically with the d4 local moments of the Mn3+ ions and become itinerant, thus aligning the Mn moments ferromagnetically. The changes in the electronic structure with carrier doping are not of the rigid band type: By La substitution for SrMnO3, the so-called in-gap spectral weight (of eg symmetry) appears with its peak located 1-2 eV below the Fermi level and grows in intensity with increasing La concentration, while the spectral intensity of the eg states above the Fermi level decreases, showing a transfer of spectral weight from the unoccupied to the occupied eg states with electron doping. Meanwhile, the intensity at the Fermi level remains low even in the metallic phase (0.2x0.6). The energy shifts of core-level peaks and valence-band features with x suggest a downward shift of the Fermi level with hole doping, but the shift is found to be very small in the metallic phase. The importance of the orbital degeneracy of the eg band and possible orbital fluctuations in the ferromagnetic phase are pointed out.",
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T1 - Electronic structure of La1-xSrxMnO3 studied by photoemission and x-ray-absorption spectroscopy

AU - Saitoh, T.

AU - Bocquet, A. E.

AU - Mizokawa, Takashi

AU - Namatame, H.

AU - Fujimori, A.

AU - Abbate, M.

AU - Takeda, Y.

AU - Takano, M.

PY - 1995

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N2 - The electronic structure of La1-xSrxMnO3 has been studied by photoemission and O 1s x-ray-absorption spectroscopy. Spectra of the Mn 2p core levels and the valence bands for LaMnO3 and SrMnO3 have been analyzed using a configuration-interaction cluster model. The ground state of LaMnO3 is found to be mixed d4 and d5L states and that of SrMnO3 to be heavily mixed d3 and d4L states, reflecting their strong covalency. The character of the band gap of LaMnO3 is of the p-to-d charge-transfer type while that of SrMnO3 has considerable p-p character as well as p-d character. Holes doped into LaMnO3 mainly of oxygen p character are coupled antiferromagnetically with the d4 local moments of the Mn3+ ions and become itinerant, thus aligning the Mn moments ferromagnetically. The changes in the electronic structure with carrier doping are not of the rigid band type: By La substitution for SrMnO3, the so-called in-gap spectral weight (of eg symmetry) appears with its peak located 1-2 eV below the Fermi level and grows in intensity with increasing La concentration, while the spectral intensity of the eg states above the Fermi level decreases, showing a transfer of spectral weight from the unoccupied to the occupied eg states with electron doping. Meanwhile, the intensity at the Fermi level remains low even in the metallic phase (0.2x0.6). The energy shifts of core-level peaks and valence-band features with x suggest a downward shift of the Fermi level with hole doping, but the shift is found to be very small in the metallic phase. The importance of the orbital degeneracy of the eg band and possible orbital fluctuations in the ferromagnetic phase are pointed out.

AB - The electronic structure of La1-xSrxMnO3 has been studied by photoemission and O 1s x-ray-absorption spectroscopy. Spectra of the Mn 2p core levels and the valence bands for LaMnO3 and SrMnO3 have been analyzed using a configuration-interaction cluster model. The ground state of LaMnO3 is found to be mixed d4 and d5L states and that of SrMnO3 to be heavily mixed d3 and d4L states, reflecting their strong covalency. The character of the band gap of LaMnO3 is of the p-to-d charge-transfer type while that of SrMnO3 has considerable p-p character as well as p-d character. Holes doped into LaMnO3 mainly of oxygen p character are coupled antiferromagnetically with the d4 local moments of the Mn3+ ions and become itinerant, thus aligning the Mn moments ferromagnetically. The changes in the electronic structure with carrier doping are not of the rigid band type: By La substitution for SrMnO3, the so-called in-gap spectral weight (of eg symmetry) appears with its peak located 1-2 eV below the Fermi level and grows in intensity with increasing La concentration, while the spectral intensity of the eg states above the Fermi level decreases, showing a transfer of spectral weight from the unoccupied to the occupied eg states with electron doping. Meanwhile, the intensity at the Fermi level remains low even in the metallic phase (0.2x0.6). The energy shifts of core-level peaks and valence-band features with x suggest a downward shift of the Fermi level with hole doping, but the shift is found to be very small in the metallic phase. The importance of the orbital degeneracy of the eg band and possible orbital fluctuations in the ferromagnetic phase are pointed out.

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