An Attempt to Improve Understanding of the Physics behind Superconductor Phase Transitions and Stability
Harald Reiss

TL;DR
This paper investigates the physics of superconductor phase transitions and stability, emphasizing the importance of transient temperature and critical parameters, and introduces a multi-physics model to address the non-uniqueness of critical temperature during phase transitions.
Contribution
It presents a novel multi-physics model incorporating quantum mechanics and heat transfer to better understand superconductor stability and phase transition dynamics.
Findings
Transient temperature distribution can be highly non-uniform under disturbances.
Relaxation time diverges near the phase transition, questioning the uniqueness of TCrit.
Operator methods improve modeling of radiative transfer and order parameter dynamics.
Abstract
Under disturbances, superconductors may experience sudden, most undesirable phase transitions (quench) from superconducting to normal conducting state. Quench may lead to damage or even to catastrophic conductor failure. A superconductor is stable if it does not quench. Exact determination of superconductor transient, resistive states (flux flow, Ohmic) thus is mandatory to safely avoid quench. This request sharp comparison of local, transient conductor temperature and current transport density with local values of critical superconductor temperature, TCrit, and critical current density, JCrit, and the latter is a strong function of temperature. Numerical, Finite Element simulations reported previously and in this paper have provided the requested, transient temperature distribution; under disturbances, this distribution may strongly be non-uniform. But what happens if the other…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
