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Scattering of conformal higher spin fields

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abstract

We develop a formalism for describing the most general notion of tree-level scattering amplitudes in 4d conformal higher spin theory. As conformal higher spin fields obey higher-derivative equations of motion, there are many distinct on-shell external states which may contribute to their scattering, some of which grow polynomially with time, leading to ill-defined amplitudes. We characterize the set of admissible scattering states which produce finite tree amplitudes, noting that there are more such states than just standard massless higher spins obeying two-derivative equations of motion. We use conformal gravity as a prime example, where the set of scattering states includes the usual Einstein graviton and a `ghost' massless spin 1 particle. An extension of the usual spinor helicity formalism allows us to encode these scattering states efficiently in terms of `twistor-spinors'. This leads to compact momentum space expressions for all finite tree-level 3-point amplitudes of conformal higher spin theory. While some of these 3-point amplitudes vanish (including all those with only standard two-derivative higher spin external states), there are many others which are non-vanishing. We also comment on the generalization to scattering of conformal higher spins in AdS$_4$.

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hep-th 1

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2026 1

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CONDITIONAL 1

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On divergences in a four-derivative scalar field theory

hep-th · 2026-08-12 · conditional · novelty 8.0

The renormalisation of a four-derivative scalar theory is computed to three loops, IR finiteness and non-renormalisation theorems are proven, and the perfect-square theory's beta function is shown to agree with O(2) phi^4 to six loops.

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  • On divergences in a four-derivative scalar field theory hep-th · 2026-08-12 · conditional · none · ref 18 · internal anchor

    The renormalisation of a four-derivative scalar theory is computed to three loops, IR finiteness and non-renormalisation theorems are proven, and the perfect-square theory's beta function is shown to agree with O(2) phi^4 to six loops.