Anomalous dimensions at large charge in d=4 O(N) theory
Abstract
Recently it was shown that the scaling dimension of the operator φn in λ(φ*φ)2 theory may be computed semi-classically at the Wilson-Fisher fixed point in d=4-ε, for generic values of λ n and this was verified to two loop order in perturbation theory at leading and sub-leading n. In subsequent work, this result was generalised to operators of fixed charge Q in O(N) theory and verified up to three loops in perturbation theory at leading and sub-leading order. Here we extend this verification to four loops in O(N) theory, once again at leading and sub-leading order. We also investigate the strong-coupling regime.
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