FL* Interpretation of a Dichotomy in the Spin Susceptibility of the Cuprates

We propose that some dichotomic Fermi liquid versus non-Fermi liquid behaviours of physical quantities in hole-doped cuprates can be explained in terms of the FL* fractionalized Fermi liquid concept, introduced some years ago, even beyond the region of underdoping. The particle excitations of this F...

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Main Author: Pieralberto Marchetti
Format: Article
Language:English
Published: MDPI AG 2023-03-01
Series:Condensed Matter
Subjects:
Online Access:https://www.mdpi.com/2410-3896/8/2/30
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author Pieralberto Marchetti
author_facet Pieralberto Marchetti
author_sort Pieralberto Marchetti
collection DOAJ
description We propose that some dichotomic Fermi liquid versus non-Fermi liquid behaviours of physical quantities in hole-doped cuprates can be explained in terms of the FL* fractionalized Fermi liquid concept, introduced some years ago, even beyond the region of underdoping. The particle excitations of this FL* system are the holon carrying charge, the spinon carrying spin 1/2, gauge fluctuations coupling them and the hole as a spinon–holon bound state or resonance due to gauge binding. In our proposal, physical responses have a Fermi-liquid-type behaviour if they are dominated by the hole resonance, whereas a non-Fermi liquid behaviour appears if they are dominated by spinon–spinon (and possibly also holon–holon) gauge interactions. The specific case of spin susceptibility in the so-called "strange metal phase" is discussed. The uniform susceptibility turns out to be hole-dominated, the spin-lattice relaxation rate in the Cu sites is spinon-dominated.
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spelling doaj.art-2e99c85879cc438e94951355a61ab4612023-11-18T09:54:24ZengMDPI AGCondensed Matter2410-38962023-03-01823010.3390/condmat8020030FL* Interpretation of a Dichotomy in the Spin Susceptibility of the CupratesPieralberto Marchetti0Dipartimento di Fisica e Astronomia, Università di Padova, INFN, I-35131 Padova, ItalyWe propose that some dichotomic Fermi liquid versus non-Fermi liquid behaviours of physical quantities in hole-doped cuprates can be explained in terms of the FL* fractionalized Fermi liquid concept, introduced some years ago, even beyond the region of underdoping. The particle excitations of this FL* system are the holon carrying charge, the spinon carrying spin 1/2, gauge fluctuations coupling them and the hole as a spinon–holon bound state or resonance due to gauge binding. In our proposal, physical responses have a Fermi-liquid-type behaviour if they are dominated by the hole resonance, whereas a non-Fermi liquid behaviour appears if they are dominated by spinon–spinon (and possibly also holon–holon) gauge interactions. The specific case of spin susceptibility in the so-called "strange metal phase" is discussed. The uniform susceptibility turns out to be hole-dominated, the spin-lattice relaxation rate in the Cu sites is spinon-dominated.https://www.mdpi.com/2410-3896/8/2/30cupratesfractionalized Fermi liquid<i>t-J</i> model
spellingShingle Pieralberto Marchetti
FL* Interpretation of a Dichotomy in the Spin Susceptibility of the Cuprates
Condensed Matter
cuprates
fractionalized Fermi liquid
<i>t-J</i> model
title FL* Interpretation of a Dichotomy in the Spin Susceptibility of the Cuprates
title_full FL* Interpretation of a Dichotomy in the Spin Susceptibility of the Cuprates
title_fullStr FL* Interpretation of a Dichotomy in the Spin Susceptibility of the Cuprates
title_full_unstemmed FL* Interpretation of a Dichotomy in the Spin Susceptibility of the Cuprates
title_short FL* Interpretation of a Dichotomy in the Spin Susceptibility of the Cuprates
title_sort fl interpretation of a dichotomy in the spin susceptibility of the cuprates
topic cuprates
fractionalized Fermi liquid
<i>t-J</i> model
url https://www.mdpi.com/2410-3896/8/2/30
work_keys_str_mv AT pieralbertomarchetti flinterpretationofadichotomyinthespinsusceptibilityofthecuprates