Magnetic Scaling in Superconductors
Ian D. Lawrie
DOI 10.1103/PhysRevLett.79.131 · Physical Review Letters
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Abstract
The Ginzburg-Landau-Wilson superconductor in a magnetic field B is considered in the approximation that magnetic-field fluctuations are neglected. A formulation of perturbation theory is presented in which multiloop calculations fully retaining all Landau levels are tractable. A 2-loop calculation shows that, near the zero-field critical point, the singular part of the free energy scales as Fsing≈|t|2−αF(B|t|−2ν), where ν is the coherence-length exponent—a result which has hitherto been assumed on purely dimensional grounds.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| YBaCuO Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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