Instability of baryonic black branes

A bstract Baryonic black branes describe the quantum critical phase of the conformal conifold gauge theory at strong coupling. This phase extends to zero temperature at a finite baryonic chemical potential, represented by extremal black branes with AdS 2 × R 3 × T 1,1 throat in asymptotic AdS 5 × T 1,1 geometry. We demonstrate here that this phase is dynamically unstable below some critical value of T c / μ : the instability is represented by a diffusive mode in the hydrodynamic sound channel with a negative diffusion coefficient. We also identify a new (exotic) ordered phase of the conifold gauge theory: this phase originates at the same critical value of T c / μ , but extends to arbitrary high temperatures, and is characterized by an expectation value of a dimension-2 operator, $$ {\mathcal{O}}_2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>O</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:math> ∝ T 2 , in the limit $$ \frac{\mu }{T} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mfrac> <mml:mi>μ</mml:mi> <mml:mi>T</mml:mi> </mml:mfrac> </mml:math> → 0.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-05-27
DOI
https://doi.org/10.1007/jhep05(2025)215
Citations
3
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
5.61

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article

Instability of baryonic black branes

Alex Buchel
3 citations
Journal of High Energy Physics
Black Holes and Theoretical Physics
5.61
article

Instability of baryonic black branes

Alex Buchel
article en
3 citations

Abstract

A bstract Baryonic black branes describe the quantum critical phase of the conformal conifold gauge theory at strong coupling. This phase extends to zero temperature at a finite baryonic chemical potential, represented by extremal black branes with AdS 2 × R 3 × T 1,1 throat in asymptotic AdS 5 × T 1,1 geometry. We demonstrate here that this phase is dynamically unstable below some critical value of T c / μ : the instability is represented by a diffusive mode in the hydrodynamic sound channel with a negative diffusion coefficient. We also identify a new (exotic) ordered phase of the conifold gauge theory: this phase originates at the same critical value of T c / μ , but extends to arbitrary high temperatures, and is characterized by an expectation value of a dimension-2 operator, $$ {\mathcal{O}}_2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>O</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:math> ∝ T 2 , in the limit $$ \frac{\mu }{T} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mfrac> <mml:mi>μ</mml:mi> <mml:mi>T</mml:mi> </mml:mfrac> </mml:math> → 0.

Journal of High Energy PhysicsVol. 2025(5)
Western University (CA), Perimeter Institute (CA)
Government of Canada, Industry Canada, Institut Périmètre de physique théorique, Natural Sciences and Engineering Research Council of Canada
Openalex Percentile: Top 5%
Black Holes and Theoretical Physics
5.61
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