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Enumerating higher-dimensional operators with on-shell amplitudes

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arxiv 1912.08827 v3 pith:GLLEUENJ submitted 2019-12-18 hep-ph hep-th

classification hep-phhep-th
keywords operatorsstructuresamplitudesdimensionhelicityindependentinvolvingon-shell
verification ladder T0 review T1 audit T2 compute T3 formal

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We establish a simple formula for the minimal dimension of operators leading to any helicity amplitude. It eases the systematic enumeration of independent operators from the construction of massless non-factorizable on-shell amplitudes. Little-group constraints can then be solved algorithmically for each helicity configuration to extract a complete set of spinor structures with lowest dimension. Occasionally, further reduction using momentum conservation, on-shell conditions and Schouten identities is required. A systematic procedure to account for the latter is presented. Dressing spinor structures with dot products of momenta finally yields the independent Lorentz structures for each helicity amplitude. We apply these procedures to amplitudes involving particles of spins 0,1/2,1,2. Spin statistics and elementary selection rules due to gauge symmetry lead to an enumeration of operators involving gravitons and standard-model particles, in the effective field theory denoted GRSMEFT. We also list the independent spinor structures generated by operators involving standard-model particles only. In both cases, we cover operators of dimension up to eight.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Massive Helicity-Chirality Spinor Formalism from Massless Amplitudes with On-shell Mass Insertion

    hep-ph 2025-01 conditional novelty 7.0 of 10

    A new helicity-chirality spinor basis with a 'transversality' charge claims a one-to-one UV-IR correspondence between massive amplitudes and massless amplitudes with Higgs insertions, and reproduces pion decay, top de...

  2. Non-factorizable Superamplitudes for Massive N = 1 Superstates

    hep-th 2025-05 conditional novelty 6.0 of 10

    Massive N=1 superamplitudes for chiral multiplets have the universal non-factorizable form δ^(2)(Q†) Q^2 ∏(1 - 1/2 η_i^2), with form factors built from Q and Q† insertions.

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