The overdoped end of the cuprate phase diagram
arXiv:2004.13120 · doi:10.1103/PhysRevResearch.2.033132
Abstract
Studying the disappearance of superconductivity at the end of the overdoped region of the cuprate phase diagram offers a different approach for investigating the interaction which is responsible for pairing in these materials. In the underdoped region this question is complicated by the presence of charge and stripe ordered phases as well as the pseudogap. In the overdoped region the situation appears simpler with only a normal phase, a superconducting phase and impurity scattering. Here, for the overdoped region, we report the results of a combined dynamic cluster approximation (DCA) and a weak Born impurity scattering calculation for a Hubbard model. We find that a decrease in the -wave pairing strength of the two-particle scattering vertex is closely coupled to changes in the momentum and frequency structure of the magnetic spin fluctuations as the system is overdoped. Treating the impurity scattering within a disordered BCS -wave approximation, we see how the combined effects of the decreasing -wave pairing strength and weak impurity scattering lead to the end of the dome.
arXiv comment5 pages, 5 figures
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- Effect of realistic out-of-plane dopant potentials on the superfluid density of overdoped cuprates
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- Effect of on-site Coulomb repulsion on ferromagnetic fluctuations in heavily over-doped cuprates
- Transport properties of very overdoped nonsuperconducting Bi2Sr2CuO6+d thin films
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- Dynamic Parallel Spin Stripes from the 1/8 anomaly to the End of Superconductivity in LaNdSrCuO
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