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Temperature dependence of lower critical field Hc1(T) shows nodeless superconductivity in FeSe

M. Abdel-Hafiez, J. Ge, A. N. Vasiliev, D. A. Chareev, J. Van de Vondel, V. V. Moshchalkov, A. V. Silhanek

DOI 10.1103/PhysRevB.88.174512 · Physical Review B

T1

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Abstract

We investigate the temperature dependence of the lower critical field Hc1(T) of a high-quality FeSe single crystal under static magnetic fields H parallel to the c axis. The temperature dependence of the first vortex penetration field has been experimentally obtained by two independent methods and the corresponding Hc1(T) was deduced by taking into account demagnetization factors. A pronounced change in the Hc1(T) curvature is observed, which is attributed to anisotopic s-wave or multiband superconductivity. The London penetration depth λab(T) calculated from the lower critical field does not follow an exponential behavior at low temperatures, as it would be expected for a fully gapped clean s-wave superconductor. Using either a two-band model with s-wave-like gaps of magnitudes Δ1=0.41±0.1 meV and Δ2=3.33±0.25 meV or a single anisotropic s-wave order parameter, the temperature dependence of the lower critical field Hc1(T) can be well described. These observations clearly show that the superconducting energy gap in FeSe is nodeless.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
FeSe

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9.4Pressure unresolvedonset
FeSe

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9.4Pressure unresolvedunknown
FeSe

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8Pressure unresolvedunknown
FeSe

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36.78.9 GPaunknown
FeSe0.85

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—Pressure not reportedunknown

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