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Absolute values of ρab (300 K) for three representative Co concentrations are 0.676 mΩcm (x=0, undoped), 0.906 mΩcm (x=0.061, optimally doped), and 0.696 mΩcm (x=0.18, completely overdoped).
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Absolute values of ρab (300 K) for three representative Co concentrations are 0.676 mΩcm (x=0, undoped), 0.906 mΩcm (x=0.061, optimally doped), and 0.696 mΩcm (x=0.18, completely overdoped).
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The origin of the significant difference between the resistivity anomaly associated with the structural/magnetic transitions in undoped BaFe2 As2 and Co-doped BaFe2 As2 is unclear. Recent optical conductivity measurements indicate that a substantial fraction of the FS of BaFe2 As2 is gapped below the SDW transition (Ref.). In this case, we can speculate that there is a subtle balance between effects associated with the reduction in the number of carriers and changes in the scattering. We note that the resistivity anomaly associated with the magnetic/structural phase transitions observed for intermediate Co concentrations is reminiscent of that which is observed for BaFe2 As2 grown from a Sn flux (Ref.), possibly indicating that Sn substitution also affects the scattering in a similarly sensitive manner.
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The origin of the significant difference between the resistivity anomaly associated with the structural/magnetic transitions in undoped BaFe2 As2 and Co-doped BaFe2 As2 is unclear. Recent optical conductivity measurements indicate that a substantial fraction of the FS of BaFe2 As2 is gapped below the SDW transition (Ref.). In this case, we can speculate that there is a subtle balance between effects associated with the reduction in the number of carriers and changes in the scattering. We note that the resistivity anomaly associated with the magnetic/structural phase transitions observed for intermediate Co concentrations is reminiscent of that which is observed for BaFe2 As2 grown from a Sn flux (Ref.), possibly indicating that Sn substitution also affects the scattering in a similarly sensitive manner.
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