Weak coupling large-N transitions at finite baryon density

TL;DR

This paper investigates large-N gauge theories with baryon chemical potential, revealing novel third-order phase transitions linked to baryon melting and Bose condensation of squarks, through a holomorphic matrix integral approach.

Contribution

It introduces a new analysis of large-N gauge theories with scalar flavors, identifying third-order deconfining phase transitions driven by baryon degeneracy.

Findings

Discovery of third-order deconfining phase transitions.

Identification of baryon melting into (s)quarks.

Phase boundary indicating Bose condensation of squarks.

Abstract

We study thermodynamics of free SU(N) gauge theory with a large number of colours and flavours on a three-sphere, in the presence of a baryon number chemical potential. Reducing the system to a holomorphic large-N matrix integral, paying specific attention to theories with scalar flavours (squarks), we identify novel third-order deconfining phase transitions as a function of the chemical potential. These transitions in the complex large-N saddle point configurations are interpreted as "melting" of baryons into (s)quarks. They are triggered by the exponentially large (~ exp(N)) degeneracy of light baryon-like states, which include ordinary baryons, adjoint-baryons and baryons made from different spherical harmonics of flavour fields on the three-sphere. The phase diagram of theories with scalar flavours terminates at a phase boundary where baryon number diverges, representing the onset of Bose condensation of squarks.