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Deconfinement transitions in a generalised XY model

Authors :
Pablo Serna
J. T. Chalker
Paul Fendley
Laboratoire de Physique Statistique de l'ENS (LPS)
Fédération de recherche du Département de physique de l'Ecole Normale Supérieure - ENS Paris (FRDPENS)
École normale supérieure - Paris (ENS Paris)
Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS Paris)
Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)
Université Paris Diderot - Paris 7 (UPD7)
Université Pierre et Marie Curie - Paris 6 (UPMC)
Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS Paris)-Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS Paris)-Université Paris Diderot - Paris 7 (UPD7)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)
École normale supérieure - Paris (ENS-PSL)
Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-École normale supérieure - Paris (ENS-PSL)
Source :
J.Phys.A, J.Phys.A, 2017, 50 (42), pp.424003. ⟨10.1088/1751-8121/aa89a1⟩
Publication Year :
2017
Publisher :
arXiv, 2017.

Abstract

We find the complete phase diagram of a generalised XY model that includes half-vortices. The model possesses superfluid, pair-superfluid and disordered phases, separated by Kosterlitz-Thouless (KT) transitions for both the half-vortices and ordinary vortices, as well as an Ising-type transition. There also occurs an unusual deconfining phase transition, where the disordered to superfluid transition is of Ising rather than KT type. We show by analytical arguments and extensive numerical simulations that there is a point in the phase diagram where the KT transition line meets the deconfining Ising phase transition. We find that the latter extends into the disordered phase not as a phase transition, but rather solely as a deconfinement transition. It is best understood in the dual height model, where on one side of the transition height steps are bound into pairs while on the other they are unbound. We also extend the phase diagram of the dual model, finding both O(2) loop model and antiferromagnetic Ising transitions.<br />Comment: 19 pages. v2: references added and minor changes. Appears in "John Cardy's scale-invariant journey in low dimensions: a special issue for his 70th birthday"

Details

Database :
OpenAIRE
Journal :
J.Phys.A, J.Phys.A, 2017, 50 (42), pp.424003. ⟨10.1088/1751-8121/aa89a1⟩
Accession number :
edsair.doi.dedup.....ab1c1619506c5d687b11ae4aec3a6f50
Full Text :
https://doi.org/10.48550/arxiv.1706.01475