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In this paper, we prove that the “conformal collider bounds” originally proposed in 1 hold for any unitary parity-preserving conformal field theory (CFT) with a unique stress tensor in dimensions d ≥ 3. In particular this implies that the ratio of central charges for a unitary 4d CFT lies in the interval 3118 ac 13. For superconformal theories this is further reduced to 32 ac 12. The proof relies only on CFT first principles — in particular, bootstrap methods — and thus constitutes the first complete field theory proof of these bounds. We further elaborate on similar bounds for non-conserved currents and relate them to results obtained recently from deep inelastic scattering.
Hofman et al. (Wed,) studied this question.