Quasiparticle spin susceptibility in heavy-fermion superconductors : An NMR study compared with specific heat results
arXiv:cond-mat/0308562 · doi:10.1143/JPSJ.74.1245
Abstract
Quasi-particle spin susceptibility () for various heavy-fermion (HF) superconductors are discussed on the basis of the experimental results of electronic specific heat (), NMR Knight shift () and NMR relaxation rate () within the framework of the Fermi liquid model for a Kramers doublet crystal electric field (CEF) ground state. is calculated from the enhanced Sommerfeld coefficient and from the quasi-particle Korringa relation via the relation of where is the hyperfine coupling constant, the Abogadoro's number and the Bohr magneton. For the even-parity (spin-singlet) superconductors CeCuSi, CeCoIn and UPdAl, the fractional decrease in the Knight shift, , below the superconducting transition temperature () is due to the decrease of the spin susceptibility of heavy quasi-particle estimated consistently from and . This result allows us to conclude that the heavy quasi-particles form the spin-singlet Cooper pairs in CeCuSi, CeCoIn and UPdAl. On the other hand, no reduction in the Knight shift is observed in UPt and UNiAl, nevertheless the estimated values of and are large enough to be probed experimentally. The odd-parity superconductivity is therefore concluded in these compounds. The NMR result provides a convincing way to classify the HF superconductors into either even- or odd- parity paring together with the identification for the gap structure, as long as the system has Kramers degeneracy.
11 pages, 3 tables, 5 figures, RevTex4(LaTex2e)
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