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Electronic States and Superconductivity in Alkali-Intercalated Fullerides:<sup>13</sup>C-NMR Study in Na<sub>2</sub>RbC<sub>60</sub>, Na<sub>2</sub>CsC<sub>60</sub>, K<sub>3</sub>C<sub>60</sub>, K<sub>2</sub>RbC<sub>60</sub>, K<sub>2</sub>CsC<sub>60</sub>, KRbCsC<sub>60</sub>, Rb<sub>2</sub>CsC<sub>60</sub>and RbCs<sub>2</sub>C<sub>60</sub>
34
Citations
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References
1994
Year
Superconducting MaterialCharge ExcitationsEngineeringBismuth-based SuperconductorsSolid-state ChemistryChemistryRelevant Phonon EnergyElectronic StructureNovel SuperconductorsElectronic StatesSuperconductivityQuantum MaterialsSuperconducting DevicesMaterials ScienceInorganic ChemistryHigh-tc SuperconductivityPhysicsC Nmr ExperimentSolid-state PhysicSystematic 13SpintronicsAlkali-intercalated FulleridesHigh-temperature SuperconductivityNatural SciencesCondensed Matter PhysicsApplied PhysicsPhononQuantum Superconductivity
A systematic 13 C NMR experiment is reported in alkali-fullerides A 3 C 60 (where A 3 is alkali-metals) between superconducting transition temperature T c and ∼100 K. Careful 13 C NMR spin-lattice relaxation time study clarified the properties of the conduction electron wave functions at Fermi surface. An upper limit of Stoner exchange parameter was estimated to be ∼3 eV/(spin-carbon), which is far from spin-wave instability criterion. Based on these studies, a variation of the density of states at Fermi level, N ( E f ), with T c was deduced. The results were analyzed in terms of McMillan formula, leading to weak or medium electron-phonon coupling constants and relevant phonon energy larger than 600 K. It was strongly suggested that the A 3 C 60 superconductor is described within a framework of the conventional phonon-mediated BCS superconductivity.
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