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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

T1

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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

FormulaReported Tc (K)Pressure (GPa)Type
UPt3

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0.55Pressure not reportedunknown
UPt3

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0.54Pressure not reportedonset
UPt3

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0.48Pressure not reportedmidpoint
U(Pt1-xPdx)3

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—Pressure not reportedunknown
U(Pt1-xPdx)3

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown

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