In high-Tc cuprates,many quantities exhibit a non-Fermi liquid universality hinting at a very peculiar structure of the underlying pairing mechanism for superconductivity: in this work, we focus on the universality for the in-plane resistivity and the superfluid density. We outline the previously developed spin–charge gauge approach to superconductivity in hole-doped cuprates: we decompose the hole of the t −t' − J model for the CuO2 planes as the product of a spinful, chargeless gapped spinon and a spinless, charged holon with Fermi surface. Each one of these particle excitations is bound to a statistical gauge flux, allowing one to optimize their statistics.We show that this model allows for a natural interpretation of the universality: within this approach, under suitable conditions, the spinonic and holonic contributions to a response function sum up according to the Ioffe–Larkin rule.We argue that, if the spinonic contribution dominates, then one should expect strongly non-Fermi-liquid-like universality, due to the insensitivity of spinons to Fermi surface details. The in-plane resistivity and superfluid density are indeed dominated by spinons in the underdoped region.We theoretically derive these quantities, discussing their universal behaviours and comparing them with experimental data.

Universality in Cuprates: A Gauge Approach

MARCHETTI, PIERALBERTO;BIGHIN, GIACOMO
2016

Abstract

In high-Tc cuprates,many quantities exhibit a non-Fermi liquid universality hinting at a very peculiar structure of the underlying pairing mechanism for superconductivity: in this work, we focus on the universality for the in-plane resistivity and the superfluid density. We outline the previously developed spin–charge gauge approach to superconductivity in hole-doped cuprates: we decompose the hole of the t −t' − J model for the CuO2 planes as the product of a spinful, chargeless gapped spinon and a spinless, charged holon with Fermi surface. Each one of these particle excitations is bound to a statistical gauge flux, allowing one to optimize their statistics.We show that this model allows for a natural interpretation of the universality: within this approach, under suitable conditions, the spinonic and holonic contributions to a response function sum up according to the Ioffe–Larkin rule.We argue that, if the spinonic contribution dominates, then one should expect strongly non-Fermi-liquid-like universality, due to the insensitivity of spinons to Fermi surface details. The in-plane resistivity and superfluid density are indeed dominated by spinons in the underdoped region.We theoretically derive these quantities, discussing their universal behaviours and comparing them with experimental data.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11577/3221119
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