Bose condensation and branes

TL;DR

This paper explores the thermodynamics of black holes in AdS space, linking the cosmological constant to the number of colors in the boundary gauge theory, and examines the behavior of the chemical potential for color across different phases.

Contribution

It provides a novel interpretation of varying the cosmological constant as changing the number of colors in the boundary gauge theory and calculates the associated chemical potential in AdS/CFT.

Findings

The chemical potential for color is negative at high temperatures.

It approaches zero below the Hawking-Page transition temperature.

The sign of the chemical potential changes near the phase transition.

Abstract

When the cosmological constant is considered to be a thermodynamical variable in black hole thermodynamics, analogous to a pressure, its conjugate variable can be thought of as a thermodynamic volume for the black hole. In the AdS/CFT correspondence this interpretation cannot be applied to the CFT on the boundary but, from the point of view of the boundary $SU(N)$ gauge theory, varying the cosmological constant in the bulk is equivalent to varying the number of colors in the gauge theory. This interpretation is examined in the case of $AdS_5\times S^5$, for ${\cal N}=4$ SUSY Yang-Mills at large $N$, and the variable thermodynamically conjugate to $N$, a chemical potential for color, is determined. It is shown that the chemical potential in the high temperature phase of the Yang-Mills theory is negative and decreases as temperature increases, as expected. For spherical black holes in the bulk the chemical potential approaches zero as the temperature is lowered below the Hawking-Page temperature and changes sign at a temperature that is within one part in a thousand of the temperature at which the heat capacity diverges.