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Orbitally degenerate spin-fluctuation model for heavy-fermion superconductivity

M. R. Norman

DOI 10.1103/PhysRevB.50.6904 · Physical Review B

T1

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Abstract

In this paper, a generalization of standard spin-fluctuation theory is considered by replacing the simple Hubbard interaction by the screened Hartree-Fock interaction for f electrons. This model is then used in both an LS and a JJ coupling scheme to construct the particle-particle scattering vertex. In an on-site approximation, this vertex is shown to lead to an instability for a superconducting pair state which obeys Hunds rules, with L=5, S=1, and J=4, whereas for near-neighbor pairing, the most attractive instability is for J=0. The degeneracy of these multiplets is broken by anisotropy of the quasiparticle wave functions. Detailed calculations are presented for the case of UPt3.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
UPt3

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—Pressure not reportedunknown
UBe13

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—Pressure not reportedunknown
U2PtC2

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—Pressure not reportedunknown
URu2Si2

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—Pressure not reportedunknown
UPd2Al3

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—Pressure not reportedunknown
UNi2Al3

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—Pressure not reportedunknown
CeCu2Si2

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—Pressure not reportedunknown

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