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Spin anisotropy due to spin-orbit coupling in optimally hole-doped Ba_(0.67)K_(0.33)Fe₂As₂

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arxiv 1612.00379 v2 pith:RQPFGUSZ submitted 2016-12-01 cond-mat.supr-con cond-mat.str-el

Spin anisotropy due to spin-orbit coupling in optimally hole-doped Ba_(0.67)K_(0.33)Fe₂As₂

classification cond-mat.supr-con cond-mat.str-el
keywords anisotropyspinironoptimallybafeconnectioncouplingelectron-doped
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We use polarized inelastic neutron scattering to study the temperature and energy dependence of spin space anisotropies in the optimally hole-doped iron pnictide Ba$_{0.67}$K$_{0.33}$Fe$_{2}$As$_{2}$ ($T_{{\rm c}}=38$ K). In the superconducting state, while the high-energy part of the magnetic spectrum is nearly isotropic, the low-energy part displays a pronouced anisotropy, manifested by a $c$-axis polarized resonance. We also observe that the spin anisotropy in superconducting Ba$_{0.67}$K$_{0.33}$Fe$_{2}$As$_{2}$ extends to higher energies compared to electron-doped BaFe$_{2-x}TM_{x}$As$_{2}$ ($TM=$Co, Ni) and isovalent-doped BaFe$_{2}$As$_{1.4}$P$_{0.6}$, suggesting a connection between $T_{\rm c}$ and the energy scale of the spin anisotropy. In the normal state, the low-energy spin anisotropy for optimally hole- and electron-doped iron pnictides onset at temperatures similar to the temperatures at which the elastoresistance deviate from Curie-Weiss behavior, pointing to a possible connection between the two phenomena. Our results highlight the relevance of the spin-orbit coupling to the superconductivity of the iron pnictides.

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