Triple critical point and emerging temperature scales in SU(N) ferromagnetism at large N

The non-Abelian ferromagnet recently introduced by the authors, consisting of atoms in the fundamental representation of SU(N), is studied in the limit where N becomes large and scales as the square root of the number of atoms n. This model exhibits additional phases, as well as two different temperature scales related by a factor N/ln⁡N. The paramagnetic phase splits into a “dense” and a “dilute” phase, separated by a third-order transition and leading to a triple critical point in the scale parameter n/N2 and the temperature, while the ferromagnetic phase exhibits additional structure, and a new paramagnetic-ferromagnetic metastable phase appears at the larger temperature scale. These phases can coexist, becoming stable or metastable as temperature varies. A generalized model in which the number of SU(N)-equivalent states enters the partition function with a nontrivial weight, relevant, e.g., when there is gauge invariance in the system, is also studied and shown to manifest similar phases, the dense-dilute phase transition becoming second-order in the fully gauge invariant case.

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Publication Details

Journal
Nuclear Physics B
Published
2024-11-19
DOI
https://doi.org/10.1016/j.nuclphysb.2024.116748
Citations
2
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
1.32

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article

Triple critical point and emerging temperature scales in SU(N) ferromagnetism at large N

Konstantinos Sfetsos, Alexios P. Polychronakos
2 citations
Nuclear Physics B
Quantum Chromodynamics and Particle Interactions
1.32
article

Triple critical point and emerging temperature scales in SU(N) ferromagnetism at large N

Konstantinos Sfetsos, Alexios P. Polychronakos
article en
2 citations

Abstract

The non-Abelian ferromagnet recently introduced by the authors, consisting of atoms in the fundamental representation of SU(N), is studied in the limit where N becomes large and scales as the square root of the number of atoms n. This model exhibits additional phases, as well as two different temperature scales related by a factor N/ln⁡N. The paramagnetic phase splits into a “dense” and a “dilute” phase, separated by a third-order transition and leading to a triple critical point in the scale parameter n/N2 and the temperature, while the ferromagnetic phase exhibits additional structure, and a new paramagnetic-ferromagnetic metastable phase appears at the larger temperature scale. These phases can coexist, becoming stable or metastable as temperature varies. A generalized model in which the number of SU(N)-equivalent states enters the partition function with a nontrivial weight, relevant, e.g., when there is gauge invariance in the system, is also studied and shown to manifest similar phases, the dense-dilute phase transition becoming second-order in the fully gauge invariant case.

Nuclear Physics BVol. 1009
National Science Foundation, CERN, Directorate for Mathematical and Physical Sciences, Research Foundation of The City University of New York
Climate action
Openalex Percentile: Top 10%
Quantum Chromodynamics and Particle Interactions
1.32
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