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Now you are in the subtree of High-Temperatures Superconductivity project. 

Attachments

  • Lower panels: plots of effective carrier density vs. doping in LSCO (left) and YBCO (right). The open squares are obtained from integrating the optical conductivity to $650\textrm{ cm}^{-1}\approx 80$~meV (lower points) and to $10,000\textrm{ cm}^{-1}\approx1.25$~eV (upper points). The filled circles show the density of carriers determined from the Hall coefficient $R_{\rm H}$ measured at 250 K (lower points) and at 720 K (upper points). Upper panels: estimates of the effective mass. From Padilla {\it et al.} \cite{padi05}.
  • Lower panels: plots of effective carrier density vs. doping in LSCO (left) and YBCO (right). The open squares are obtained from integrating the optical conductivity to $650\textrm{ cm}^{-1}\approx 80$~meV (lower points) and to $10,000\textrm{ cm}^{-1}\approx1.25$~eV (upper points). The filled circles show the density of carriers determined from the Hall coefficient $R_{\rm H}$ measured at 250 K (lower points) and at 720 K (upper points). Upper panels: estimates of the effective mass. From Padilla {\it et al.} \cite{padi05}.
  • fig_eff_carrier.jpeg