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The phase diagrams and the nature of the phase transitions in multicomponent gauge theories with an Abelian gauge field are important topics with various physical applications. While an early renormalization-group-based study indicated that the direct transition from a fully ordered to a fully disordered state is continuous for <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:mi>N</a:mi><a:mo>=</a:mo><a:mn>1</a:mn></a:mrow></a:math> and <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:mrow><b:mi>N</b:mi><b:mo>></b:mo><b:mn>183</b:mn></b:mrow></b:math>, recently it was demonstrated that the transition is discontinuous for <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:mrow><c:mi>N</c:mi><c:mo>=</c:mo><c:mn>2</c:mn></c:mrow></c:math>. We quantitatively study the dependence on <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:mi>N</d:mi></d:math> of the degree of discontinuity of this transition. Our results suggest that the transition is discontinuous at least up to <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:mrow><e:mi>N</e:mi><e:mo>=</e:mo><e:mn>7</e:mn></e:mrow></e:math>. Furthermore, we demonstrate that, at increased coupling strength, the phase transitions of the neutral and charged sectors of the model split, which for <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:mrow><f:mi>N</f:mi><f:mo>></f:mo><f:mn>2</f:mn></f:mrow></f:math> yields a new phase with composite order. The transition from the composite-order phase to the fully disordered phase is then also discontinuous, at least for <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:mrow><g:mi>N</g:mi><g:mo>=</g:mo><g:mn>3</g:mn></g:mrow></g:math> and <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:mi>N</h:mi><h:mo>=</h:mo><h:mn>4</h:mn></h:mrow></h:math>. Via a duality argument, this indicates that van der Waals–type interaction between directed loops may be responsible for the discontinuous phase transitions in these models.
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Weston et al. (2024) studied this question.
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