Superconducting stiffness
ρs and coherence length
ξ are usually determined by measuring the penetration depth
λ of a magnetic field and the upper critical field
Hc2 of a superconductor (SC), respectively. However, in magnetic SC, which is iron-based, this could
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Superconducting stiffness
ρs and coherence length
ξ are usually determined by measuring the penetration depth
λ of a magnetic field and the upper critical field
Hc2 of a superconductor (SC), respectively. However, in magnetic SC, which is iron-based, this could lead to erroneous results, since the internal field could be very different from the applied one. To overcome this problem in Fe
1+ySe
xTe
1−x with
x∼0.5 and
y∼0 (FST), we measured both quantities with the Stiffnessometer technique. In this technique, one applies a rotor-free vector potential
A to a superconducting ring and measures the current density
j via the ring’s magnetic moment
m.
ρs and
ξ are determined from London’s equation,
j=−ρsA, and its range of validity. This method is particularly accurate at temperatures close to the critical temperature
Tc. We find weaker
ρs and longer
ξ than existing literature reports, and critical exponents which agree better with expectations based on the Ginzburg–Landau theory.
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