Superconducting classes of heavy-fermion materials
Masa-aki Ozaki, Kazushige Machida
DOI 10.1103/PhysRevB.39.4145 · Physical Review B
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Abstract
Stimulated by recent remarkable findings which lead to a common feature of all four known heavy-fermion superconductors UPt3, (U,Th)Be13, URu2Si2, and CeCu2Si2, namely, a close proximity between the magnetism and unconventional superconducting pairing state we present a general framework on how to identify the superconducting classes. Taking into account the existence of the spin-density wave (SDW) above Tc in UPt3 and URu2Si2 and below Tc in (U,Th)Be13 and CeCu2Si2, we enumerate group theoretically the pairing states compatible with given space-group symmetry according to the Landau subordination scheme for the second-order phase transition. This enables us to effectively narrow down the possible states. These enumerated states are quite general, independent of particular models or pairing interaction forms. Then we give some physical arguments on the relative stability among the allowed states. Maximally utilizing experimental and theoretical data available at present, we attempt to decrease the number of the possible states and obtain the most plausible candidates for each material. To confirm the emerging universal feature that the ground state in heavy-fermion superconductors is the coexisting phase with the magnetism, further experiments are proposed, based on our results.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| UPt3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.5 | Pressure not reported | unknown |
| CeCu2Si2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.6 | Pressure not reported | unknown |
| URu2Si2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1 | Pressure not reported | unknown |
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