Spin cones in random-field XY models

Fuente: arXiv
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Auteurs principaux: Pereira, Rajiv G, Janardhanan, Ananya, Barma, Mustansir
Format: Preprint
Publié: 2024
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author Pereira, Rajiv G
Janardhanan, Ananya
Barma, Mustansir
author_facet Pereira, Rajiv G
Janardhanan, Ananya
Barma, Mustansir
contents We determine the arrangement of spins in the ground state of the XY model with quenched, random fields, on a fully connected graph. Two types of disordered fields are considered, namely randomly oriented magnetic fields, and randomly oriented crystal fields. Orientations are chosen from a uniformly isotropic distribution, but disorder fluctuations in each realization of a finite system lead to a breaking of rotational symmetry. The result is an interesting pattern of spin orientations, found by solving a system of coupled, nonlinear equations within perturbation theory and also by exact numerical continuation. All spins lie within a cone for small enough ratio of field to coupling strength, with an interesting distribution of spin orientations, with peaks at the cone edges. The orientation of the cone depends strongly on the realization of disorder, but the opening angle does not. In the case of random magnetic fields, the cone angle widens as the ratio increases till a critical value at which there is a first order phase transition and the cone disappears. With random crystal fields, there is no phase transition and the cone angle approaches $180^\circ$ for large values of the ratio. At finite low temperatures, Monte-Carlo simulations show that the formation of a cone and its subsequent alignment along the equilibrium direction occur on two different time scales.
format Preprint
id arxiv_https___arxiv_org_abs_2403_19939
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Spin cones in random-field XY models
Pereira, Rajiv G
Janardhanan, Ananya
Barma, Mustansir
Statistical Mechanics
Disordered Systems and Neural Networks
We determine the arrangement of spins in the ground state of the XY model with quenched, random fields, on a fully connected graph. Two types of disordered fields are considered, namely randomly oriented magnetic fields, and randomly oriented crystal fields. Orientations are chosen from a uniformly isotropic distribution, but disorder fluctuations in each realization of a finite system lead to a breaking of rotational symmetry. The result is an interesting pattern of spin orientations, found by solving a system of coupled, nonlinear equations within perturbation theory and also by exact numerical continuation. All spins lie within a cone for small enough ratio of field to coupling strength, with an interesting distribution of spin orientations, with peaks at the cone edges. The orientation of the cone depends strongly on the realization of disorder, but the opening angle does not. In the case of random magnetic fields, the cone angle widens as the ratio increases till a critical value at which there is a first order phase transition and the cone disappears. With random crystal fields, there is no phase transition and the cone angle approaches $180^\circ$ for large values of the ratio. At finite low temperatures, Monte-Carlo simulations show that the formation of a cone and its subsequent alignment along the equilibrium direction occur on two different time scales.
title Spin cones in random-field XY models
topic Statistical Mechanics
Disordered Systems and Neural Networks
url https://arxiv.org/abs/2403.19939