The ordered phase of charged N=4 SYM plasma

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1. Verfasser: Buchel, Alex
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Veröffentlicht: 2025
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author Buchel, Alex
author_facet Buchel, Alex
contents Recently is has been shown \cite{Gladden:2024ssb} that strongly coupled ${\cal N}=4$ supersymmetric Yang-Mills plasma with diagonal $U(1)$ $R$-charge chemical potential is unstable at $\fracμ{2πT}=\sqrt{2}$. We construct a new homogeneous and isotropic phase of this plasma that dominates in the microcanonical ensemble (but not in the grand canonical one). The new phase extends to arbitrary high temperatures, \ie as $T\gg μ$, and is characterized by an expectation value of a dimension-2 operator, with ${\cal O}_2\propto T^2$ -- it is the {\it ordered conformal phase}. In the limit $\fracμT\to 0$, this ordered phase has vanishing energy density $\frac{\cal E}{T^4}\propto \frac{μ^2}{T^2}$ and is a low entropy density state $\frac{\cal S}{T^3}\propto \frac{μ^2}{T^2}$.
format Preprint
id arxiv_https___arxiv_org_abs_2501_01856
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle The ordered phase of charged N=4 SYM plasma
Buchel, Alex
High Energy Physics - Theory
Recently is has been shown \cite{Gladden:2024ssb} that strongly coupled ${\cal N}=4$ supersymmetric Yang-Mills plasma with diagonal $U(1)$ $R$-charge chemical potential is unstable at $\fracμ{2πT}=\sqrt{2}$. We construct a new homogeneous and isotropic phase of this plasma that dominates in the microcanonical ensemble (but not in the grand canonical one). The new phase extends to arbitrary high temperatures, \ie as $T\gg μ$, and is characterized by an expectation value of a dimension-2 operator, with ${\cal O}_2\propto T^2$ -- it is the {\it ordered conformal phase}. In the limit $\fracμT\to 0$, this ordered phase has vanishing energy density $\frac{\cal E}{T^4}\propto \frac{μ^2}{T^2}$ and is a low entropy density state $\frac{\cal S}{T^3}\propto \frac{μ^2}{T^2}$.
title The ordered phase of charged N=4 SYM plasma
topic High Energy Physics - Theory
url https://arxiv.org/abs/2501.01856