Superconductivity in heavy-fermion U(Pt,Pd)3 and its interplay with magnetism
R. J. Keizer, A. de Visser, M. J. Graf, A. A. Menovsky, J. J. M. Franse
DOI 10.1103/PhysRevB.60.10527 · 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
The effect of Pd doping on the superconducting phase diagram of the unconventional superconductor UPt3 has been measured by (magneto)resistance, specific heat, thermal expansion, and magnetostriction. Experiments on single- and polycrystalline U(Pt1−xPdx)3 for x<~0.006 show that the superconducting transition temperatures of the A phase Tc+, and of the B phase Tc− both decrease, while the splitting ΔTc increases at a rate of 0.30±0.02K/at.% Pd. The B phase is suppressed first, near x=0.004, while the A phase survives until x≅0.007. We find that ΔTc(x) correlates with an increase of the weak magnetic moment m(x) upon Pd doping. This provides further evidence for Ginzburg-Landau scenarios with magnetism as the symmetry-breaking field, i.e., the two-dimensional (2D) E representation and the 1D odd-parity model. Only for small splittings ΔTc∝m2(Tc+) (ΔTc<~0.05K) as predicted. The results at larger splittings call for Ginzburg-Landau expansions beyond fourth order. The tetracritical point in the B-T plane persists until at least x=0.002 for B⊥c, while it is rapidly suppressed for B∥c. Upon alloying the A and B phases gain stability at the expense of the C phase.
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. | 0.55 | Pressure not reported | unknown |
| UPt3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.54 | Pressure not reported | onset |
| UPt3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 0.48 | Pressure not reported | midpoint |
| U(Pt1-xPdx)3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| U(Pt1-xPdx)3 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 0.95Matthias J. Graf & Daryl W. Hess
Source status unknown — claims are unverified
Anisotropic temperature dependence of the magnetic-field penetration in superconducting UPt3
similarity 0.95C. Broholm et al.
Source status unknown — claims are unverified
Lower and upper critical fields in the heavy electron superconductor UPt3
similarity 0.95B. S. Shivaram et al.
Source status unknown — claims are unverified
Magnetic properties of UPt3 in the superconducting state
similarity 0.95Andreas Amann et al.
Source status unknown — claims are unverified
Possible superconductivity in nearly antiferromagnetic itinerant fermion systems
similarity 0.95M. T. Béal-Monod et al.
Source status unknown — claims are unverified
Spin susceptibility of the topological superconductor UPt3 from polarized neutron diffraction
similarity 0.95W. J. Gannon et al.
Source status unknown — claims are unverified