Bootstrapping Mixed Correlators in the Five Dimensional Critical O(N) Models
Zhijin Li, Ning Su
TL;DR
This work uses a mixed-correlator conformal bootstrap approach to study five-dimensional $O(N)$ vector CFTs, focusing on the leading vector $\phi_i$ and singlet $\sigma$. By combining crossing symmetry with unitarity and imposing dimension gaps, the authors carve out islands in the $(Δ_φ,Δ_σ)$ plane, finding a small island for $N=500$ that matches large-$N$ predictions and shrinks with increasing derivation order $Λ$. For $N\le100$, islands appear only at low $Λ$ and vanish at higher $Λ$, implying a critical value $N_c>100$ and suggesting the interacting fixed point becomes nonunitary below $N_c$. Overall, the results provide nonperturbative, high-precision constraints on 5D $O(N)$ CFT data and support a large-$N$ unitary fixed point while highlighting potential nonunitarity at smaller $N$.
Abstract
We use the conformal bootstrap approach to explore $5D$ CFTs with $O(N)$ global symmetry, which contain $N$ scalars $φ_i$ transforming as $O(N)$ vector. Specifically, we study multiple four-point correlators of the leading $O(N)$ vector $φ_i$ and the $O(N)$ singlet $σ$. The crossing symmetry of the four-point functions and the unitarity condition provide nontrivial constraints on the scaling dimensions ($Δ_φ$, $Δ_σ$) of $φ_i$ and $σ$. With reasonable assumptions on the gaps between scaling dimensions of $φ_i$ ($σ$) and the next $O(N)$ vector (singlet) scalar, we are able to isolate the scaling dimensions $(Δ_φ$, $Δ_σ)$ in small islands. In particular, for large $N=500$, the isolated region is highly consistent with the result obtained from large $N$ expansion. We also study the interacting $O(N)$ CFTs for $1\leqslant N\leqslant100$. Isolated regions on $(Δ_φ,Δ_σ)$ plane are obtained using conformal bootstrap program with lower order of derivatives $Λ$; however, they disappear after increasing $Λ$. We think these islands are corresponding to interacting but nonunitary $O(N)$ CFTs. Our results provide a lower bound on the critical value $N_c>100$, below which the interacting $O(N)$ CFTs turn into nonunitary. The critical value is unexpectedly large comparing with previous estimations.
