Superconductivity mediated by spin fluctuations in the heavy-fermion compound UPd2Al3
Nature. Bd. 398. H. 6722. 1999 S. 47 - 49
Erscheinungsjahr: 1999
ISBN/ISSN: 0028-0836
Publikationstyp: Zeitschriftenaufsatz
Sprache: Englisch
Doi/URN: 10.1038/17977
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Inhaltszusammenfassung
It is well known that any weak attractive electron±electron interaction in metals can in principle cause the formation of Cooper pairs, which then condense into a superconducting ground state1. In conventional superconductors, this attractive interaction is mediated by lattice vibrations (phonons). But for the heavy-fermion and high-temperature superconductors, alternative pairing interactions are considered to be possible2. For example, the low-temperature properties of heavy-fermion ...It is well known that any weak attractive electron±electron interaction in metals can in principle cause the formation of Cooper pairs, which then condense into a superconducting ground state1. In conventional superconductors, this attractive interaction is mediated by lattice vibrations (phonons). But for the heavy-fermion and high-temperature superconductors, alternative pairing interactions are considered to be possible2. For example, the low-temperature properties of heavy-fermion systems are dominated by antiferromagnetic spin Fluctuations, which have been considered theoretically3 as a possible cause for Cooper-pair formation. This picture recently received some experimental support: the resistivity behaviour under pressure of two cerium-based heavy-fermion compounds was shown to be consistent with a magnetically mediated pairing mechanism4. Here we use tunnelling spectroscopy to investigate the superconducting order parameter of a uranium-based heavy-fermion superconductorÐepitaxial thin ®lms of UPd2Al3. Our observation of a strong-coupling feature in the tunnelling conductivity, combined with recent inelastic neutron scattering data13±15 strongly suggest a pairing interaction mediated by spin Fluctuations.» weiterlesen» einklappen
Klassifikation
DFG Fachgebiet:
Physik der kondensierten Materie
DDC Sachgruppe:
Physik