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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.

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FormulaReported Tc (K)Pressure (GPa)Type
YBaCuO

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—Pressure not reportedunknown

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