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Magnetic anisotropy in hole-doped superconducting Ba0.67K0.33Fe2As2 probed by polarized inelastic neutron scattering

Chenglin Zhang, Mengshu Liu, Yixi Su, Louis-Pierre Regnault, Meng Wang, Guotai Tan, Th. Brückel, Takeshi Egami, Pengcheng Dai

DOI 10.1103/PhysRevB.87.081101 · Physical Review B

T1

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Abstract

We use polarized inelastic neutron scattering (INS) to study spin excitations of optimally hole-doped superconductor Ba0.67K0.33Fe2As2 (Tc=38 K). In the normal state, the imaginary part of the dynamic susceptibility, χ′′(Q,ω), shows magnetic anisotropy for energies below ∼7 meV with c-axis polarized spin excitations larger than that of the in-plane component. Upon entering into the superconducting state, previous unpolarized INS experiments have shown that spin gaps at ∼5 and 0.75 meV open at wave vectors Q=(0.5,0.5,0) and (0.5,0.5,1), respectively, with a broad neutron spin resonance at Er=15 meV. Our neutron polarization analysis reveals that the large difference in spin gaps is purely due to different spin gaps in the c axis and in-plane polarized spin excitations, resulting in a resonance with different energy widths for the c-axis and in-plane spin excitations. The observation of spin anisotropy in both optimally electron- and hole-doped BaFe2As2 is due to their proximity to the AF ordered BaFe2As2 where spin anisotropy exists below TN.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Ba0.67K0.33Fe2As2

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38Pressure not reportedunknown
YBa2Cu3O6.9

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93Pressure not reportedunknown
Pr0.88LaCe0.12CuO4-δ

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—Pressure not reportedunknown
BaFe1.9Ni0.1As2

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20Pressure not reportedunknown
BaFe1.85Ni0.15As2

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14Pressure not reportedunknown
BaFe1.88Co0.12As2

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24Pressure not reportedunknown

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