Self-energy driven resonancelike inelastic neutron spectrum in the s++-wave state in Fe-based superconductors
Lisa Takeuchi, Youichi Yamakawa, Hiroshi Kontani
DOI 10.1103/PhysRevB.98.165143 · Physical Review B
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Abstract
To elucidate the pairing states in Fe-based superconductors, we perform a careful calculation of the dynamical spin susceptibility χS(q,ω) at very low temperatures (T≳1meV). The feedback effect on both the self-energy and χS(q,ω) from the superconducting gap is self-consistently analyzed based on the fluctuation-exchange (FLEX) approximation. In the s±-wave state, which has sign reversal in the gap function, χS(q,ω) at the nesting momentum q=Q shows a resonance peak even when the system is away from the magnetic quantum critical point (QCP). In the s++-wave state that has no sign reversal, χS(q,ω) shows a large hump structure when the system is close to the magnetic QCP. This result confirms the validity of a self-energy driven resonancelike peak in the s++-wave state proposed in our previous semimicroscopic study: The enhancement in χS(q,ω) due to the self-energy effect exceeds the suppression due to the coherence factor effect near the magnetic QCP. We stress that the hump structure in the s++-wave state given by the FLEX method smoothly changes to a resonancelike sharp peak structure as the system approaches the magnetic QCP, which was not reported in our previous studies. The obtained ω and T dependence of χS(q,ω) in the s++-wave states resembles the resonancelike feature in inelastic neutron scattering spectra recently observed in Na(Fe,Co)As and FeSe.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Na(Fe,Co)As Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| FeSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| CeCoIn5 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| MgB2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| YNi2B2C Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| BaFe2-xCoxAs2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| (Ba,K)Fe2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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