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Fully gapped superconductivity in the topological superconductor β−PdBi2

P. K. Biswas, D. G. Mazzone, R. Sibille, E. Pomjakushina, K. Conder, H. Luetkens, C. Baines, J. L. Gavilano, M. Kenzelmann, A. Amato, E. Morenzoni

DOI 10.1103/PhysRevB.93.220504 · Physical Review B

T1

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Abstract

The recent discovery of the topologically protected surface states in the β phase of PdBi2 has reignited the research interest in this class of superconductors. Here, we show results of our muon spin relaxation and rotation (μSR) measurements carried out to investigate the superconducting and magnetic properties and the topological effect in the superconducting ground state of β−PdBi2. Zero-field μSR data reveal that no sizable spontaneous magnetization arises with the onset of superconductivity implying that the time reversal symmetry is preserved in the superconducting state of β−PdBi2. Further, a strong diamagnetic shift of the applied field has been observed in the transverse-field (TF) μSR experiments, indicating that any triplet-pairing channel, if present, does not dominate the superconducting condensate. Using TF-μSR, we estimate that the magnetic penetration depth λ=263(10) nm at zero temperature. The nature of λ(T) provides evidence for the existence of a nodeless single s-wave type isotropic energy gap of 0.78(1) meV at zero temperature. Our results further suggest that the topologically protected surface states have no effect on the bulk of the superconductor.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
PdBi2

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5.4Pressure not reportedonset
PdBi2

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4.84Pressure not reportedmidpoint
PdBi2

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4.25Pressure not reportedunknown
PdBi2

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1.73Pressure not reportedunknown
PdBi

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3.8Pressure not reportedunknown
Pd2.5Bi1.5

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3.7Pressure not reportedunknown

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