Polarized neutron scattering studies of magnetic excitations in electron-overdoped superconducting BaFe1.85_{1.85}Ni0.15_{0.15}As2_{2}

preprint2012arXivOpen access

Abstract

We use polarized inelastic neutron scattering to study low-energy spin excitations and their spatial anisotropy in electron-overdoped superconducting BaFe1.85_{1.85}Ni0.15_{0.15}As2_{2} (Tc=14T_c=14 K). In the normal state, the imaginary part of the dynamic susceptibility, χ′′(Q,ω)χ^{\prime\prime}(Q,ω), at the antiferromagnetic (AF) wave vector Q=(0.5,0.5,1)Q=(0.5,0.5,1) increases linearly with energy for E≤13E\le 13 meV. Upon entering the superconducting state, a spin gap opens below E≈3E\approx 3 meV and a broad neutron spin resonance appears at E≈7E\approx 7 meV. Our careful neutron polarization analysis reveals that χ′′(Q,ω)χ^{\prime\prime}(Q,ω) is isotropic for the in-plane and out-of-plane components in both the normal and superconducting states. A comparison of these results with those of undoped BaFe2_2As2_2 and optimally electron-doped BaFe1.9_{1.9}Ni0.1_{0.1}As2_{2} (Tc=20T_c=20 K) suggests that the spin anisotropy observed in BaFe1.9_{1.9}Ni0.1_{0.1}As2_{2} is likely due to its proximity to the undoped BaFe2_2As2_2. Therefore, the neutron spin resonance is isotropic in the overdoped regime, consistent with a singlet to triplet excitation.

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