Stiffnessometer, a magnetic-field-free superconducting stiffness meter and its application
arXiv:1705.00624 · doi:10.1103/PhysRevB.102.024502
Abstract
We provide a detailed account for a new method to measure superconducting stiffness , critical current density , and coherence length , in one apparatus, without subjecting the sample to magnetic field or attaching leads. The method is based on the London equation , where is the current density and is the vector potential. Using a rotor free and a measurement of via the magnetic moment of a superconducting ring, we determine . By increasing until the London equation fails we determine and . The method is sensitive to very small stiffness, which translates to penetration depth ~mm. It is also sensitive to low critical current density Amm or long coherence length ~m. Naturally, the method does not suffer from demagnetization factor complications, the presence of vortices, or out-of-equilibrium conditions. Therefore, the absolute values of the different parameters can be determined. We demonstrate the application of this method to LaSrCuO with .
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- Boundary effects in two-band superconductors
- The nature of the phase transition in the cuprates as revealed by a magnetic field free stiffness meter
- Ginzburg-Landau model of a Stiffnessometer -- a superconducting stiffness meter device
- Elevated critical temperature at BCS superconductor-band insulator interfaces
- Stiffness and coherence length measurements of ultra-thin superconductor, and implications to layered superconductors
- Superconducting Stiffness and Coherence Length of FeSeTe Measured in Zero-Applied Field
- Effect of medium on fundamental interactions in gravity and condensed matter
- The two critical temperatures conundrum in LaSrCuO