Ampère phase in frustrated magnets

Fuente: arXiv
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Main Authors: Rougemaille, N., Coraux, J., Canals, B.
Format: Preprint
Published: 2025
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author Rougemaille, N.
Coraux, J.
Canals, B.
author_facet Rougemaille, N.
Coraux, J.
Canals, B.
contents We report a new class of algebraic spin liquids, in which the macroscopically degenerate ground state manifold is not Coulombic, like in spin ices, but Ampère-like. The local constraint characterizing an Ampère phase is not a Gauss law, but rather an Ampère law, i.e., a condition on the curl of the magnetization vector field and not on its divergence. As a consequence, the excitations evolving in such a manifold are not magnetically charged scalar quasiparticles, the so-called magnetic monopoles in Coulomb phases, but instead vectorial magnetic loops (or fictional current lines). We demonstrate analytically that in a macroscopically degenerate manifold inheriting the properties of a cooperative paramagnet and subject to a local curl-free contraint, magnetic correlations decay in space with a power law whose exponent is the space dimension d: the Ampère phase is a d-algebraic spin liquid. Using Monte Carlo simulations with appropriate cluster dynamics, we confirm this physics numerically in two- and three-dimensional examples, and illustrate how the Ampère phase compares to its Coulomb counterpart.
format Preprint
id arxiv_https___arxiv_org_abs_2501_08859
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Ampère phase in frustrated magnets
Rougemaille, N.
Coraux, J.
Canals, B.
Strongly Correlated Electrons
Disordered Systems and Neural Networks
Other Condensed Matter
We report a new class of algebraic spin liquids, in which the macroscopically degenerate ground state manifold is not Coulombic, like in spin ices, but Ampère-like. The local constraint characterizing an Ampère phase is not a Gauss law, but rather an Ampère law, i.e., a condition on the curl of the magnetization vector field and not on its divergence. As a consequence, the excitations evolving in such a manifold are not magnetically charged scalar quasiparticles, the so-called magnetic monopoles in Coulomb phases, but instead vectorial magnetic loops (or fictional current lines). We demonstrate analytically that in a macroscopically degenerate manifold inheriting the properties of a cooperative paramagnet and subject to a local curl-free contraint, magnetic correlations decay in space with a power law whose exponent is the space dimension d: the Ampère phase is a d-algebraic spin liquid. Using Monte Carlo simulations with appropriate cluster dynamics, we confirm this physics numerically in two- and three-dimensional examples, and illustrate how the Ampère phase compares to its Coulomb counterpart.
title Ampère phase in frustrated magnets
topic Strongly Correlated Electrons
Disordered Systems and Neural Networks
Other Condensed Matter
url https://arxiv.org/abs/2501.08859