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Cuprate pseudogap: Competing order parameters or precursor superconductivity

Jelena Stajic, Andrew Iyengar, K. Levin, B. R. Boyce, T. R. Lemberger

DOI 10.1103/PhysRevB.68.024520 · Physical Review B

T1

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Abstract

In this paper we compare two broad classes of theories for the pseudogap in cuprate superconductors. The comparison is made in reference to measurements of the superfluid density ρs(T,x) in YBa2CuO7−δ films having a wide range of stoichiometries δ or, hole doping, x. The theoretical challenge raised by these (and previous) data is to understand why the T dependence of ρs(T,x) is insensitive to the fermionic excitation gap Δ(T,x), which opens in the normal state and persists into the superconducting state, when presumably ρs(T) is governed, at least in part, by fermionic excitations. Indeed, ρs(T,x) seems to have a BCS-like scaling with Tc(x), which, although not unexpected, is not straightforward to understand in pseudogapped superconductors where Tc(x) and the excitation gap have little in common. Here, we contrast “extrinsic” and “intrinsic” theoretical approaches to the pseudogap and argue that the former (for example, associated with a competing order parameter) exhibits more obvious departures from BCS-like T dependences in ρs(T) than approaches, which associate the pseudogap with the superconductivity itself. Examples of the latter are the Fermi-liquid-based schemes as well as a pair fluctuation mean-field theory. Thus far, the measured behavior of the superfluid density appears to argue against an extrinsic interpretation of the pseudogap, and supports instead its intrinsic origin.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
YBa2Cu3O7-δ

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—Pressure not reportedunknown
YBa2Cu3O7

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown

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