Massive Higher-Spin Fields in the Fractional Quantum Hall Effect

Fuente: arXiv
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Autores principales: Bergshoeff, Eric, Campoleoni, Andrea, Palumbo, Giandomenico, Salgado-Rebolledo, Patricio
Formato: Preprint
Publicado: 2024
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author Bergshoeff, Eric
Campoleoni, Andrea
Palumbo, Giandomenico
Salgado-Rebolledo, Patricio
author_facet Bergshoeff, Eric
Campoleoni, Andrea
Palumbo, Giandomenico
Salgado-Rebolledo, Patricio
contents Incompressibility plays a key role in the geometric description of fractional quantum Hall fluids. It is naturally related to quantum area-preserving diffeomorphisms and the underlying Girvin-MacDonald-Plazman algebra, which gives rise to an emergent non-relativistic massive spin-2 mode propagating in the bulk. The corresponding metric tensor can be identified with a nematic order parameter for the bulk states. In the linearised regime with a flat background, it has been shown that this mode can be described by a spin-2 Schroedinger action. However, quantum area-preserving diffeomorphisms also suggest the existence of higher-spin modes that cannot be described through nematic fractional quantum Hall states. Here, we consider p-atic Hall phases, in which the corresponding p-atic order parameters are related to higher-rank symmetric tensors. We then show that in this framework, non-relativistic massive chiral higher-spin fields naturally emerge and that their dynamics is described by higher-spin Schroedinger actions. We finally show that these effective actions can be derived from relativistic massive higher-spin theories in 2+1 dimensions after taking a non-relativistic limit.
format Preprint
id arxiv_https___arxiv_org_abs_2404_16013
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Massive Higher-Spin Fields in the Fractional Quantum Hall Effect
Bergshoeff, Eric
Campoleoni, Andrea
Palumbo, Giandomenico
Salgado-Rebolledo, Patricio
Strongly Correlated Electrons
Mesoscale and Nanoscale Physics
High Energy Physics - Theory
Incompressibility plays a key role in the geometric description of fractional quantum Hall fluids. It is naturally related to quantum area-preserving diffeomorphisms and the underlying Girvin-MacDonald-Plazman algebra, which gives rise to an emergent non-relativistic massive spin-2 mode propagating in the bulk. The corresponding metric tensor can be identified with a nematic order parameter for the bulk states. In the linearised regime with a flat background, it has been shown that this mode can be described by a spin-2 Schroedinger action. However, quantum area-preserving diffeomorphisms also suggest the existence of higher-spin modes that cannot be described through nematic fractional quantum Hall states. Here, we consider p-atic Hall phases, in which the corresponding p-atic order parameters are related to higher-rank symmetric tensors. We then show that in this framework, non-relativistic massive chiral higher-spin fields naturally emerge and that their dynamics is described by higher-spin Schroedinger actions. We finally show that these effective actions can be derived from relativistic massive higher-spin theories in 2+1 dimensions after taking a non-relativistic limit.
title Massive Higher-Spin Fields in the Fractional Quantum Hall Effect
topic Strongly Correlated Electrons
Mesoscale and Nanoscale Physics
High Energy Physics - Theory
url https://arxiv.org/abs/2404.16013