Plasma-Plasma Third Order Phase Transition from Type IIB Supergravity

We show that the planar, charged black hole in asymptotically anti-de Sitter spacetime, dual to the strongly coupled quark-gluon plasma thermal state of large N, SU(N), N=4 super Yang-Mills at finite chemical potential undergoes a third-order phase transition in the grand canonical ensemble to a hairy black hole of type IIB supergravity. The hairy phase is another strongly coupled fluid with a conformal equation of state and can be interpreted as another kind of quark-gluon plasma. This new quark-gluon plasma has less entropy and, therefore, seems to characterize some form of smooth hadronization. The locus of the transition in terms of the critical values of the "baryon" chemical potential μ_{c} and the temperature T_{c} is μ_{c}=2πT_{c}.

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Publication Details

Journal
Physical Review Letters
Published
2024-09-19
DOI
https://doi.org/10.1103/physrevlett.133.121601
Citations
7
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
4.62

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article

Plasma-Plasma Third Order Phase Transition from Type IIB Supergravity

Andrès Anabalòn, Julio Oliva
7 citations
Physical Review Letters
Black Holes and Theoretical Physics
4.62
article

Plasma-Plasma Third Order Phase Transition from Type IIB Supergravity

Andrès Anabalòn, Julio Oliva
article en
7 citations

Abstract

We show that the planar, charged black hole in asymptotically anti-de Sitter spacetime, dual to the strongly coupled quark-gluon plasma thermal state of large N, SU(N), N=4 super Yang-Mills at finite chemical potential undergoes a third-order phase transition in the grand canonical ensemble to a hairy black hole of type IIB supergravity. The hairy phase is another strongly coupled fluid with a conformal equation of state and can be interpreted as another kind of quark-gluon plasma. This new quark-gluon plasma has less entropy and, therefore, seems to characterize some form of smooth hadronization. The locus of the transition in terms of the critical values of the "baryon" chemical potential μ_{c} and the temperature T_{c} is μ_{c}=2πT_{c}.

Physical Review LettersVol. 133(12)
University of Concepción (CL)
Fondo Nacional de Desarrollo Científico y Tecnológico
Openalex Percentile: Top 4%
Black Holes and Theoretical Physics
4.62
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