TY - JOUR
T1 - Absence of superconductivity in the hole-doped Fe pnictide Ba(Fe 1-xMnx)2As2
T2 - Photoemission and x-ray absorption spectroscopy studies
AU - Suzuki, H.
AU - Yoshida, T.
AU - Ideta, S.
AU - Shibata, G.
AU - Ishigami, K.
AU - Kadono, T.
AU - Fujimori, A.
AU - Hashimoto, M.
AU - Lu, D. H.
AU - Shen, Z. X.
AU - Ono, K.
AU - Sakai, E.
AU - Kumigashira, H.
AU - Matsuo, M.
AU - Sasagawa, T.
PY - 2013/9/3
Y1 - 2013/9/3
N2 - We have studied the electronic structure of Ba(Fe1-xMn x)2As2 (x=0.08), which fails to become a superconductor in spite of the formal hole doping like Ba1-xK xFe2As2, with photoemission spectroscopy and x-ray absorption spectroscopy (XAS). With decreasing temperature, a transition from the paramagnetic phase to the antiferromagnetic phase was clearly observed by angle-resolved photoemission spectroscopy. XAS results indicated that the substituted Mn atoms form a strongly hybridized ground state. Resonance-photoemission spectra at the Mn L3 edge revealed that the Mn 3d partial density of states is distributed over a wide energy range of 2-13 eV below the Fermi level (EF), with little contribution around E F. This indicates that the dopant Mn 3d states are localized in spite of the strong Mn 3d-As 4p hybridization and split into the occupied and unoccupied parts due to the on-site Coulomb and exchange interaction. The absence of superconductivity in Ba(Fe1-xMnx) 2As2 can thus be ascribed both to the absence of carrier doping in the FeAs plane and to the stabilization of the competing G-type antiferromagnetic order by the Mn impurities.
AB - We have studied the electronic structure of Ba(Fe1-xMn x)2As2 (x=0.08), which fails to become a superconductor in spite of the formal hole doping like Ba1-xK xFe2As2, with photoemission spectroscopy and x-ray absorption spectroscopy (XAS). With decreasing temperature, a transition from the paramagnetic phase to the antiferromagnetic phase was clearly observed by angle-resolved photoemission spectroscopy. XAS results indicated that the substituted Mn atoms form a strongly hybridized ground state. Resonance-photoemission spectra at the Mn L3 edge revealed that the Mn 3d partial density of states is distributed over a wide energy range of 2-13 eV below the Fermi level (EF), with little contribution around E F. This indicates that the dopant Mn 3d states are localized in spite of the strong Mn 3d-As 4p hybridization and split into the occupied and unoccupied parts due to the on-site Coulomb and exchange interaction. The absence of superconductivity in Ba(Fe1-xMnx) 2As2 can thus be ascribed both to the absence of carrier doping in the FeAs plane and to the stabilization of the competing G-type antiferromagnetic order by the Mn impurities.
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U2 - 10.1103/PhysRevB.88.100501
DO - 10.1103/PhysRevB.88.100501
M3 - Article
AN - SCOPUS:84884861754
SN - 0163-1829
VL - 88
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 10
M1 - 100501
ER -