Superconductivity and antiferromagnetism in heavy-electron systems
Rikio Konno, Kazuo Ueda
DOI 10.1103/PhysRevB.40.4329 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
Superconductivity and antiferromagnetism in heavy-electron systems are investigated from a general point of view. First we classify superconducting states in a simple cubic lattice, a body-centered tetragonal lattice, and a hexagonal close-packed lattice, having URu2Si2 and UPt3 in mind. For that purpose we take an approach to treat the effective couplings in real space. The approach is convenient to discuss the relation between the nature of fluctuations in the system and the superconducting states. When we assume that the antiferromagnetic fluctuations reported by neutron experiments are dominant, the most promising are some of the anisotropic singlet states and there remains the possibility for some triplet states too. Then we discuss the coupling between the two order parameters based on a Ginzburg-Landau theory. We derive a general expression of the coupling term. It is pointed out that the coupling constant can be large in heavy-electron systems. The general trend of the coexistence of the superconductivity and antiferromagnetism is discussed, and it is shown that the anisotropic states are generally more favorable to the coexistence than the conventional isotropic singlet. Experimental data of URu2Si2 and UPt3 are analyzed by the Ginzburg-Landau theory. According to the analysis URu2Si2 has a small coupling constant and a large condensation energy of the antiferromagnetism. On the other hand, UPt3 has a large coupling constant and a small condensation energy. It means that the specific-heat anomaly at TN should be small in UPt3 and its superconductivity is easily destroyed when a large moment is formed.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| URu2Si2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.5 | Pressure not reported | unknown |
| 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. | 0.7 | Pressure not reported | unknown |
| CeCu2.02Si2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.72 | Pressure not reported | unknown |
| UBe13 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Antiferromagnetic domains and superconductivity in UPt3
similarity 0.98Matthias J. Graf & Daryl W. Hess
Source status unknown — claims are unverified
Superconductivity and spin-density waves: Application to heavy-fermion materials
similarity 0.97Masaru Kato & Kazushige Machida
Source status unknown — claims are unverified
Quantum critical scaling and superconductivity in heavy electron materials
similarity 0.97Yi-feng Yang et al.
Source status unknown — claims are unverified
Fluctuation effects in heavy-fermion and high-Tc superconductors
similarity 0.97E. J. Blagoeva et al.
Source status unknown — claims are unverified
Superconductivity and spin-density waves in heavy-fermion systems
similarity 0.97M. Gulácsi & Zs. Gulácsi
Source status unknown — claims are unverified
Transport processes in heavy-fermion superconductors
similarity 0.96C. J. Pethick & David Pines
Source status unknown — claims are unverified