Interplay between unconventional superconductivity and heavy-fermion quantum criticality: CeCuSi versus YbRhSi
arXiv:1808.02277 · doi:10.1080/14786435.2018.1511070
Abstract
In this paper the low-temperature properties of two isostructural canonical heavy-fermion compounds are contrasted with regards to the interplay between antiferromagnetic (AF) quantum criticality and superconductivity. For CeCuSi, fully-gapped d-wave superconductivity forms in the vicinity of an itinerant three-dimensional heavy-fermion spin-density-wave (SDW) quantum critical point (QCP). Inelastic neutron scattering results highlight that both quantum critical SDW fluctuations as well as Mott-type fluctuations of local magnetic moments contribute to the formation of Cooper pairs in CeCuSi. In YbRhSi, superconductivity appears to be suppressed at mK by AF order ( = 70 mK). Ultra-low temperature measurements reveal a hybrid order between nuclear and 4f-electronic spins, which is dominated by the Yb-derived nuclear spins, to develop at slightly above 2 mK. The hybrid order turns out to strongly compete with the primary 4f-electronic order and to push the material towards its QCP. Apparently, this paves the way for heavy-fermion superconductivity to form at = 2 mK. Like the pressure - induced QCP in CeRhIn, the magnetic field - induced one in YbRhSi is of the local Kondo-destroying variety which corresponds to a Mott-type transition at zero temperature. Therefore, these materials form the link between the large family of about fifty low- unconventional heavy - fermion superconductors and other families of unconventional superconductors with higher s, notably the doped Mott insulators of the cuprates, organic charge-transfer salts and some of the Fe-based superconductors. Our study suggests that heavy-fermion superconductivity near an AF QCP is a robust phenomenon.
arXiv comment30 pages, 7 Figures, Accepted for publication in Philosophical Magazine
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