Overdoped end of the cuprate phase diagram

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...

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Main Authors: Thomas A. Maier, Seher Karakuzu, Douglas J. Scalapino
Format: Article
Language:English
Published: American Physical Society 2020-07-01
Series:Physical Review Research
Online Access:http://doi.org/10.1103/PhysRevResearch.2.033132
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author Thomas A. Maier
Seher Karakuzu
Douglas J. Scalapino
author_facet Thomas A. Maier
Seher Karakuzu
Douglas J. Scalapino
author_sort Thomas A. Maier
collection DOAJ
description 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 t-t^{′}-U Hubbard model. We find that a decrease in the d-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 d-wave approximation, we see how the combined effects of the decreasing d-wave pairing strength and weak impurity scattering lead to the end of the T_{c} dome.
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spelling doaj.art-ab6e9d6f379d43da82108443e920f5992024-04-12T16:57:39ZengAmerican Physical SocietyPhysical Review Research2643-15642020-07-012303313210.1103/PhysRevResearch.2.033132Overdoped end of the cuprate phase diagramThomas A. MaierSeher KarakuzuDouglas J. ScalapinoStudying 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 t-t^{′}-U Hubbard model. We find that a decrease in the d-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 d-wave approximation, we see how the combined effects of the decreasing d-wave pairing strength and weak impurity scattering lead to the end of the T_{c} dome.http://doi.org/10.1103/PhysRevResearch.2.033132
spellingShingle Thomas A. Maier
Seher Karakuzu
Douglas J. Scalapino
Overdoped end of the cuprate phase diagram
Physical Review Research
title Overdoped end of the cuprate phase diagram
title_full Overdoped end of the cuprate phase diagram
title_fullStr Overdoped end of the cuprate phase diagram
title_full_unstemmed Overdoped end of the cuprate phase diagram
title_short Overdoped end of the cuprate phase diagram
title_sort overdoped end of the cuprate phase diagram
url http://doi.org/10.1103/PhysRevResearch.2.033132
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