Theory of dual fermion superconductivity in hole-doped cuprates
Jun Chang, Jize Zhao

TL;DR
This paper presents a dual fermion model explaining the phase diagram of hole-doped cuprates, including strange metal behavior, pseudogap formation, and d-wave superconductivity, emphasizing high-energy spin fluctuations as the pairing mechanism.
Contribution
It introduces a dual fermion theoretical framework that accounts for the complex phases of hole-doped cuprates, highlighting the role of high-energy spin excitations in superconductivity.
Findings
Strange metal behavior arises from carriers in copper antiferromagnetic spin fluctuations.
High-energy spin excitations act as the 'magnetic glue' for d-wave pairing.
The pseudogap results from carrier localization or a crossover to a Kondo-like insulator.
Abstract
Since the discovery of the cuprate high-temperature superconductivity in 1986, a universal phase diagram has been constructed experimentally and numerous theoretical models have been proposed. However, there remains no consensus on the underlying physics thus far. Here, we theoretically investigate the phase diagram of hole-doped cuprates based on an itinerant-localized dual fermion model, with the charge carriers doped on the oxygen sites and localized holes on the copper orbitals. We analytically demonstrate that the puzzling anomalous normal state or the strange metal could simply stem from a free Fermi gas of carriers bathing in copper antiferromagnetic spin fluctuations. The short-range high-energy spin excitations also act as the `magnetic glue' of carrier Cooper pairs and induce -wave superconductivity from the underdoped to overdoped regime, distinctly…
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