An investigation of the in-plane dc fluctuation conductivity of optimally doped and overdoped cuprates: implication and origin of the pseudogap

TL;DR

This study investigates the in-plane fluctuation conductivity in cuprates to understand the pseudogap's origin, finding evidence that suggests the pseudogap is not related to precursor pairing but has a different origin.

Contribution

The paper provides experimental evidence differentiating the pseudogap from superconducting fluctuations in cuprates, highlighting its non-pairing origin through analysis of fluctuation conductivity.

Findings

Overdoped sample's excess conductivity fits Gaussian Ginzburg-Landau theory.

Optimally doped sample shows additional conductivity not explained by standard theory.

Results suggest the pseudogap is not due to precursor pairing.

Abstract

In conventional superconductors the magnitude of the pairing fluctuation is primarily determined by Tc and the superconducting (SC) coherence length, {\xi}. In systems with strong structural and electronic anisotropies, the interlayer separation, s, plays a significant role. In cuprates, the pseudogap (PG) correlation induces a downturn in the temperature dependent resistivity. As Tc is approached from above, this downturn in the resistivity is supposed to either i) add to or ii) join smoothly to that due to paraconductivity caused by short-lived Cooper pairs. It is important to differentiate between these two possibilities since they are closely linked to the origin of the PG. It would be reasonable to assume that if the first scenario is correct then the PG has a non-SC origin, while the second scenario, if found to hold, would relate precursor pairing to the PG correlations. We have studied the in-plane fluctuation conductivity of two c-axis oriented thin films of Y0.95Ca0.05Ba2Cu3O7-d with similar hole contents (p), p = 0.165 (optimally doped) and p = 0.184 (slightly overdoped). The hole contents are fixed at these values so that the PG affects the resistivity data only at temperatures close to Tc. Analysis of paraconductivity, {\Delta}{\sigma}ab(T), within the mean-field Gaussian Ginzburg-Landau (MFGGL) framework reveals different features for the optimally doped (OPD) and the slightly overdoped (SOD) compounds. The excess conductivity due to Cooper pair fluctuations of the SOD sample can be described reasonably well by the MFGGL formalism. The excess conductivity of the OPD compound, on the other hand, cannot be accounted for by the MFGGL formalism with reasonable set of parameters. There is a significant added contribution to {\Delta}{\sigma}ab(T) for the OPD sample which appears to come from the presence of a PG. These findings point towards a non-pairing origin of the PG.