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Anisotropic spin fluctuations in detwinned FeSe.


ABSTRACT: Superconductivity in FeSe emerges from a nematic phase that breaks four-fold rotational symmetry in the iron plane. This phase may arise from orbital ordering, spin fluctuations or hidden magnetic quadrupolar order. Here we use inelastic neutron scattering on a mosaic of single crystals of FeSe, detwinned by mounting on a BaFe2As2 substrate to demonstrate that spin excitations are most intense at the antiferromagnetic wave vectors QAF?=?(±1, 0) at low energies E?=?6-11?meV in the normal state. This two-fold (C2) anisotropy is reduced at lower energies, 3-5?meV, indicating a gapped four-fold (C4) mode. In the superconducting state, however, the strong nematic anisotropy is again reflected in the spin resonance (E?=?3.6?meV) at QAF with incommensurate scattering around 5-6?meV. Our results highlight the extreme electronic anisotropy of the nematic phase of FeSe and are consistent with a highly anisotropic superconducting gap driven by spin fluctuations.

SUBMITTER: Chen T 

PROVIDER: S-EPMC7895486 | biostudies-literature | 2019 Jul

REPOSITORIES: biostudies-literature

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Superconductivity in FeSe emerges from a nematic phase that breaks four-fold rotational symmetry in the iron plane. This phase may arise from orbital ordering, spin fluctuations or hidden magnetic quadrupolar order. Here we use inelastic neutron scattering on a mosaic of single crystals of FeSe, detwinned by mounting on a BaFe<sub>2</sub>As<sub>2</sub> substrate to demonstrate that spin excitations are most intense at the antiferromagnetic wave vectors Q<sub>AF</sub> = (±1, 0) at low energies E   ...[more]

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