2020
DOI: 10.1007/s40766-019-0001-1
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Iron-based superconductors: tales from the nuclei

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Cited by 11 publications
(6 citation statements)
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“…To stabilize of a non-zero superconducting parameter order, Anderson's above-mentioned argument about the two atoms per unit cell proves critical. We argued that a tRVB state is consistent with the body of available experimental data, from Knight shift [56], quasi-particle interference [57,58] and neutron spinresonance measurements [9]. Moreover, a tRVB order parameter is relatively robust against disorder and predicts staggered component to the pair wavefunction that, we argued, will be discernible using scanning Josephson spectroscopy.…”
Section: Introductionsupporting
confidence: 75%
“…To stabilize of a non-zero superconducting parameter order, Anderson's above-mentioned argument about the two atoms per unit cell proves critical. We argued that a tRVB state is consistent with the body of available experimental data, from Knight shift [56], quasi-particle interference [57,58] and neutron spinresonance measurements [9]. Moreover, a tRVB order parameter is relatively robust against disorder and predicts staggered component to the pair wavefunction that, we argued, will be discernible using scanning Josephson spectroscopy.…”
Section: Introductionsupporting
confidence: 75%
“…In Figure 8, the magnitude of the gap (shown by the colormap) is represented on a generic Fermi surface consisting of two tubular Fermi sheets in the first Brillouin zone for two cases: when the d-wave gap value exceeds the s-wave gap (panel a, below T * ) and for the opposite situation (panel b, above T * ). It is clear the tetragonal symmetry is lost that in both cases and only twofold symmetry is retained, as occurs in the nematic state [40]. Moreover, the order parameter is nodal only at low temperature, and the system shows a transition to a fully gapped order parameter at T * .…”
Section: Resultsmentioning
confidence: 94%
“…and it is taken when ω µ τ c = 1. Assuming ∆ ∼ 10 G as typical value for the fluctuating magnetic field induced by the motion of vortices [36] and B µ ∼ 1 kG as lower bound for the magnetic field at the muon site, we estimate λ V −AV L max ∼ 8.5 × 10 −3 µs −1 as upper-bound value of the maximum relaxation rate. The typical experimental values reported for λ L in Fig.…”
Section: Discussionmentioning
confidence: 90%