Abstract

We use time-of-flight (ToF) inelastic neutron scattering (INS) spectroscopy to investigate the doping dependence of magnetic excitations across the phase diagram of NaFe1−x_{1-x}Cox_xAs with x=0,0.0175,0.0215,0.05,x=0, 0.0175, 0.0215, 0.05, and 0.110.11. The effect of electron-doping by partially substituting Fe by Co is to form resonances that couple with superconductivity, broaden and suppress low energy (E≤80E\le 80 meV) spin excitations compared with spin waves in undoped NaFeAs. However, high energy (E>80E> 80 meV) spin excitations are weakly Co-doping dependent. Integration of the local spin dynamic susceptibility χ′′(ω)χ^{\prime\prime}(ω) of NaFe1−x_{1-x}Cox_xAs reveals a total fluctuating moment of 3.6 μB2μ_B^2/Fe and a small but systematic reduction with electron doping. The presence of a large spin gap in the Co-overdoped nonsuperconducting NaFe0.89_{0.89}Co0.11_{0.11}As suggests that Fermi surface nesting is responsible for low-energy spin excitations. These results parallel Ni-doping evolution of spin excitations in BaFe2−x_{2-x}Nix_xAs2_2, confirming the notion that low-energy spin excitations coupling with itinerant electrons are important for superconductivity, while weakly doping dependent high-energy spin excitations result from localized moments.

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