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- W137755950 abstract "For untwinned single-crystal ${mathrm{YBa}}_{2}$${mathrm{Cu}}_{3}$${mathrm{O}}_{7mathrm{ensuremath{-}}mathrm{ensuremath{delta}}}$ in a magnetic field H, we find that the in-plane Hall conductivity ${mathrm{ensuremath{sigma}}}_{mathit{x}mathit{y}}$ just below the superconducting transition temperature ${mathit{T}}_{mathit{c}}$ is the sum of two terms, ${mathit{C}}_{1}$/H and ${mathit{C}}_{2}$H, where ${mathit{C}}_{1}$ and ${mathit{C}}_{2}$ are field independent, in agreement with recent theoretical predictions of Dorsey et al. and Kopnin et al. ${mathit{C}}_{1}$ and ${mathit{C}}_{2}$ have opposite signs, as required by the observation that the Hall effect changes sign as the applied field is varied. ${mathit{C}}_{1}$ is proportional to ${mathrm{ensuremath{tau}}}^{2}$, and ${mathit{C}}_{2}$ is approximately proportional to ensuremath{tau}, where ensuremath{tau}=(${mathit{T}}_{mathit{c}}$-T)/${mathit{T}}_{mathit{c}}$, so the crossover field ${mathit{H}}_{0}$, where ${mathrm{ensuremath{sigma}}}_{mathit{x}mathit{y}}$=0, is proportional to ${mathrm{ensuremath{tau}}}^{1/2}$." @default.
- W137755950 created "2016-06-24" @default.
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- W137755950 date "1995-08-01" @default.
- W137755950 modified "2023-10-18" @default.
- W137755950 title "Erratum: Sign reversal of the Hall effect in untwinned single-crystal superconductingYBa2Cu3O7−δ" @default.
- W137755950 doi "https://doi.org/10.1103/physrevb.52.3802.2" @default.
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