# Partition function of free conformal fields in 3-plet representation

## TL;DR

This paper investigates the partition function of free conformal fields in the 3-plet representation, revealing a phase transition at very low temperature with critical temperature decreasing as 1/ log N, and discusses implications for large N theories.

## Contribution

It introduces the computation of the singlet partition function for 3-plet representation fields and analyzes its unique large N behavior and phase transition properties.

## Key findings

- Partition function exhibits asymptotic behavior at large N.
- Critical temperature T_c approaches zero as 1/ log N.
- Phase transition occurs at very low temperature for 3-plet case.

## Abstract

Simplest examples of AdS/CFT duality correspond to free CFTs in d dimensions with fields in vector or adjoint representation of an internal symmetry group dual in the large N limit to a theory of massless or massless plus massive higher spins in AdS_{d+1}. One may also study generalizations when conformal fields belong to higher dimensional representations, i.e. carry more than two internal symmetry indices. Here we consider the case of the 3-fundamental ("3-plet") representation. One motivation is a conjectured connection to multiple M5-brane theory: heuristic arguments suggest that it may be related to an (interacting) CFT of 6d (2,0) tensor multiplets in 3-plet representation of large N symmetry group that has an AdS_7 dual. We compute the singlet partition function Z on S^1 x S^{d-1} for a free field in 3-plet representation of U(N) and analyse its novel large N behaviour. The large N limit of the low temperature expansion of Z which is convergent in the vector and adjoint cases here is only asymptotic, reflecting the much faster growth of the number of singlet operators with dimension, indicating a phase transition at very low temperature. Indeed, while the critical temperatures in the vector (T_c ~ N^a, a >0) and adjoint (T_c ~ 1) cases are finite, we find that in the 3-plet case T_c ~ 1/ log N, i.e. it approaches zero at large N. We discuss some details of large N solution for the eigenvalue distribution. Similar conclusions apply to higher p-plet representations of U(N) or O(N) and also to the free p-tensor theories invariant under [U(N)]^p or [O(N)]^p starting with p=3.