Transport properties of the metallic state of overdoped cuprate superconductors from an anisotropic marginal Fermi liquid model
Jure Kokalj, Nigel E. Hussey, Ross H. McKenzie

TL;DR
This paper models the charge transport in overdoped cuprate superconductors using an anisotropic marginal Fermi liquid self-energy, successfully explaining various experimental transport data without new parameters.
Contribution
It introduces a phenomenological self-energy model combining isotropic Fermi liquid and anisotropic marginal Fermi liquid components to describe transport properties.
Findings
Quantitative agreement with resistivity, optical conductivity, magnetoresistance, and Hall coefficient data.
Highlights the role of anisotropic scattering and Fermi surface shape in transport behavior.
Shows the Fermi liquid component dominates the Hall angle temperature dependence.
Abstract
We consider the implications of a phenomenological model self-energy for the charge transport properties of the metallic phase of the overdoped cuprate superconductors. The self-energy is the sum of two terms with characteristic dependencies on temperature, frequency, location on the Fermi surface, and doping. The first term is isotropic over the Fermi surface, independent of doping, and has the frequency and temperature dependence characteristic of a Fermi liquid. The second term is anisotropic over the Fermi surface (vanishing at the same points as the superconducting energy gap), strongly varies with doping (scaling roughly with , the superconducting transition temperature), and has the frequency and temperature dependence characteristic of a marginal Fermi liquid. Previously it has been shown this self-energy can describe a range of experimental data including angle-dependent…
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