Coupling between 4f and itinerant electrons in SmFeAsO1-xFx (0.15 < x < 0.2) superconductors: an NMR study
arXiv:1003.3798 · doi:10.1103/PhysRevB.81.100508
Abstract
F NMR measurements in SmFeAsOF, for , are presented. The nuclear spin-lattice relaxation rate increases upon cooling with a trend analogous to the one already observed in CeCuAu, a quasi two-dimensional heavy-fermion intermetallic compound with an antiferromagnetic ground-state. In particular, the behaviour of the relaxation rate either in SmFeAsOF or in CeCuAu can be described in the framework of the self-consistent renormalization theory for weakly itinerant electron systems. Remarkably, no effect of the superconducting transition on F is detected, a phenomenon which can hardly be explained within a single band model.
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References in corpus (9)
- Coexistence of the spin-density-wave and superconductivity in the (Ba,K)Fe2As2
- 19-F NMR Investigation of Iron-pnictide Superconductor LaFeAsO(0.89)F(0.11)
- CeFePO: A Heavy Fermion Metal with Ferromagnetic Correlations
- Magnetic-superconducting phase boundary of SmFeAsOF studied via muon spin rotation: Unified behavior in a pnictide family
- Local moment versus Kondo behavior of the 4f-electrons in rare-earth iron oxypnictides
- Thermal properties of SmFeAs(O1-xFx) as probe of the interplay between electrons and phonons
- X-ray spectra and electronic structure of FeAs superconductors
- Heat capacity measurements on FeAs-based compounds: a thermodynamic probe of electronic and magnetic states
- Influence of the Nd states on the magnetic behavior and the electric field gradient of the oxypnictides superconductors NdFeAsOF
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- NMR Investigation of the iron-based superconductors Ca4(Mg,Ti)3Fe2As2O8-y and Ca5(Sc,Ti)4Fe2As2O11-y
- Phase separation at the magnetic-superconducting transition in LaYFeAsOF