Electronic structure of heavily electron-doped BaFe1. 7Co0. 3As2 studied by angle-resolved photoemission
Y Sekiba, T Sato, K Nakayama… - New Journal of …, 2009 - iopscience.iop.org
New Journal of Physics, 2009•iopscience.iop.org
We have performed high-resolution angle-resolved photoemission spectroscopy on heavily
electron-doped non-superconducting (SC) BaFe 1.7 Co 0.3 As 2. We find that the two hole
Fermi surface pockets at the Brillouin zone center observed in the hole-doped
superconducting Ba 0.6 K 0.4 Fe 2 As 2 are absent or very small in this compound, while the
two electron pockets at the zone corner significantly expand due to electron doping by the
Co substitution. Comparison of the Fermi surface between non-SC and SC samples …
electron-doped non-superconducting (SC) BaFe 1.7 Co 0.3 As 2. We find that the two hole
Fermi surface pockets at the Brillouin zone center observed in the hole-doped
superconducting Ba 0.6 K 0.4 Fe 2 As 2 are absent or very small in this compound, while the
two electron pockets at the zone corner significantly expand due to electron doping by the
Co substitution. Comparison of the Fermi surface between non-SC and SC samples …
Abstract
We have performed high-resolution angle-resolved photoemission spectroscopy on heavily electron-doped non-superconducting (SC) BaFe 1.7 Co 0.3 As 2. We find that the two hole Fermi surface pockets at the Brillouin zone center observed in the hole-doped superconducting Ba 0.6 K 0.4 Fe 2 As 2 are absent or very small in this compound, while the two electron pockets at the zone corner significantly expand due to electron doping by the Co substitution. Comparison of the Fermi surface between non-SC and SC samples indicates that the coexistence of hole and electron pockets connected via the antiferromagnetic wave vector is essential in realizing the mechanism of superconductivity in the iron-based superconductors.
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