Monopole ordered phases in dipolar and nearest-neighbors Ising pyrochlore: From spin ice to the all-in–all-out antiferromagnet

We study Ising pyrochlores by means of Monte Carlo simulations. We cover a set of exchange constants ranging from the frustrated ferromagnetic case (spin-ice) to the fully-ordered “all-in–all-out” antiferromagnet in the dipolar model, reinterpreting the results—as in an ionic system—in terms of a te...

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Autores principales: Guruciaga, P. C., Grigera, Santiago Andrés, Borzi, Rodolfo Alberto
Formato: Articulo
Lenguaje:Inglés
Publicado: 2014
Materias:
Acceso en línea:http://sedici.unlp.edu.ar/handle/10915/126219
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id I19-R120-10915-126219
record_format dspace
institution Universidad Nacional de La Plata
institution_str I-19
repository_str R-120
collection SEDICI (UNLP)
language Inglés
topic Ciencias Exactas
Física
Ising pyrochlores
Monte Carlo simulations
spin ice
all-in–all-out antiferromagnet
spellingShingle Ciencias Exactas
Física
Ising pyrochlores
Monte Carlo simulations
spin ice
all-in–all-out antiferromagnet
Guruciaga, P. C.
Grigera, Santiago Andrés
Borzi, Rodolfo Alberto
Monopole ordered phases in dipolar and nearest-neighbors Ising pyrochlore: From spin ice to the all-in–all-out antiferromagnet
topic_facet Ciencias Exactas
Física
Ising pyrochlores
Monte Carlo simulations
spin ice
all-in–all-out antiferromagnet
description We study Ising pyrochlores by means of Monte Carlo simulations. We cover a set of exchange constants ranging from the frustrated ferromagnetic case (spin-ice) to the fully-ordered “all-in–all-out” antiferromagnet in the dipolar model, reinterpreting the results—as in an ionic system—in terms of a temperature vs magnetic charge density phase diagram. In spite of its spin nature and the presence of both double and single nonconserved magnetic charges, the dipolar model gives place to a phase diagram which is quite comparable with those previously obtained for on-lattice systems of electric charges, and on spin ice models with a conserved number of single magnetic charges. The contrast between these systems, to which we add results from the nearest-neighbors model, put forward other features of our phase diagram—notably, a monopole fluid with charge order at high monopole densities that persists up to arbitrarily high temperatures—that can only be explained taking into account construction constraints forced by the underlying spin degrees of freedom.
format Articulo
Articulo
author Guruciaga, P. C.
Grigera, Santiago Andrés
Borzi, Rodolfo Alberto
author_facet Guruciaga, P. C.
Grigera, Santiago Andrés
Borzi, Rodolfo Alberto
author_sort Guruciaga, P. C.
title Monopole ordered phases in dipolar and nearest-neighbors Ising pyrochlore: From spin ice to the all-in–all-out antiferromagnet
title_short Monopole ordered phases in dipolar and nearest-neighbors Ising pyrochlore: From spin ice to the all-in–all-out antiferromagnet
title_full Monopole ordered phases in dipolar and nearest-neighbors Ising pyrochlore: From spin ice to the all-in–all-out antiferromagnet
title_fullStr Monopole ordered phases in dipolar and nearest-neighbors Ising pyrochlore: From spin ice to the all-in–all-out antiferromagnet
title_full_unstemmed Monopole ordered phases in dipolar and nearest-neighbors Ising pyrochlore: From spin ice to the all-in–all-out antiferromagnet
title_sort monopole ordered phases in dipolar and nearest-neighbors ising pyrochlore: from spin ice to the all-in–all-out antiferromagnet
publishDate 2014
url http://sedici.unlp.edu.ar/handle/10915/126219
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