Abstract

Motivated by the recent progress in solving the large charge sector of conformal field theories, we revisit the mass-charge relation of boson stars asymptotic to global AdS. We construct and classify a large number of electrically charged boson star solutions in a toy model and two supergravity models arising from the $SU(3)$ and $U(1)^4$ truncation of $D=4$ $SO(8)$ gauged maximal supergravity. We find a simple ansatz for the chemical potential that can fit the numerical data in striking accuracy for the full range of charge. Combining with the first law of thermodynamics, we can then evaluate the mass as a function of the charge and obtain the free energy in the fixed charge ensemble. We show that in the toy model, the ground state can be either the extremal RN black hole or the boson stars depending on the parameter region. For the $SU(3)$ truncation, there always exists a boson star that has smaller free energy than the extremal RN black hole, in contrast to the $U(1)^4$ model where the extremal RN black hole is always the ground state. In all models, for boson star solutions with arbitrarily large charge, we show that the large charge expansion of the mass reproduces the same structure exhibited in the CFT side.

Highlights

  • When it comes to solving a physical system, it is very useful to look for a small parameter about which a systematic perturbative expansion can be carried out

  • This approach led to the discovery of soluble sectors of strongly coupled conformal field theory (CFT) at large spin [1,2,3,4,5] or large global Uð1Þ charge [6,7,8,9,10,11,12] where the spectrum of the theory simplifies

  • By using the Euclidean action technique, we can determine the free energy of the boson stars and compare it with the extremal RN-anti–de Sitter (AdS) black hole

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Summary

INTRODUCTION

When it comes to solving a physical system, it is very useful to look for a small parameter about which a systematic perturbative expansion can be carried out. By using the Euclidean action technique, we can determine the free energy of the boson stars and compare it with the extremal RN-AdS black hole This allows us to determine the ground state, or the state with the lowest scaling dimensions in the dual CFT for given global Uð1Þ charge. For the AdS boson stars, we impose the boundary condition corresponding to turning on a VEV in the dual CFT spontaneously breaking the global symmetry We use both the Euclidean action and the IyerWald formalism to establish the first law of the boson star dynamics and determine the Helmholtz free energy of the fixed charge ensemble. In order not to interrupt the discussion in the main text, we reserve many illustrative figures in Appendix E

The theory and equations
The boundary condition
Scalar hairy black holes
AdS boson stars
Numerical approaches
Euclidean action and the ground state
The dynamical first law of the AdS boson star
THE PHENOMENOGICAL TOY MODEL
The Ai series
The Bi series
General q2
The Uð1Þ4 model
The A series
The B series
The C series
CONCLUSION
Detail of the truncation
Further truncation
Full Text
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