Muon spin rotation in the magnetic and superconducting ground states of (U,Th)Be13 and (U,Th)Pt3
R. H. Heffner, D. W. Cooke, A. L. Giorgi, R. L. Hutson, M. E. Schillaci, H. D. Rempp, J. L. Smith, J. O. Willis, D. E. MacLaughlin, C. Boekema, R. L. Lichti, J. Oostens, A. B. Denison
DOI 10.1103/PhysRevB.39.11345 · Physical Review B
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Abstract
Microscopic aspects of magnetism and superconductivity have been studied in the heavy-fermion superconducting alloy systems (U,Th)Be13 and (U,Th)Pt3 using the technique of positive-muon (μ+) spin rotation and relaxation (μSR). In U1−xThxBe13, x=0.033, a striking increase of zero-field Kubo-Toyabe relaxation rate σKT is observed below the temperature Tc2≃0.4 K at which a second phase transition occurs in the superconducting state. This jump is firm evidence for the onset of weak static magnetism below Tc2. The observed increase of ∼1.5 Oe in the μ+ local field corresponds to an effective moment of 10−3–10−2 μB/U atom. The μ+ Knight shift Kμ in the normal states of U1−xThxBe13, x=0 and 0.033, is proportional to the bulk susceptibility and yields a transferred f-spin-μ+ hyperfine field of -1.99±0.12 kOe/μB. In the superconducting states of U1−xThxBe13, x=0, 0.01, and 0.033, a large reduction of the magnitude of Kμ is observed for x=0 but not for x=0.033, and an intermediate reduction is found for x=0.01. This behavior suggests (1) spin-singlet pairing in undoped UBe13, and (2) conventional reduction of the spin susceptibility suppression in (U,Th)Be13 by spin-orbit scattering from Th impurities. In undoped UPt3 small increases of σKT and the transverse-field Gaussian relaxation rate σG below ∼6 K are again evidence for the onset of weak static magnetism similar to that found in (U,Th)Be13. Recent spin-polarized neutron scattering studies of normal-state UPt3 have observed a commensurate antiferromagnetic (AF) structure with a sublattice magnetization of ∼10−2 μB/U atom, in rough agreement with the μSR results. For U1−xThxPt3, x=0.05, zero-field μ+ precession frequencies below 6.5 K indicate an AF structure with a considerably larger moment (∼0.6 μB/U atom). The average μ+ Knight shift in the normal state of undoped UPt3 is much smaller than in UBe13, which suggests multiple μ+ stopping sites with hyperfine couplings of opposite signs.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| UBe13 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| U1-xThxBe13 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.4 | Pressure not reported | unknown |
| UPt3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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