Effective field theory amplitudes the on-shell way: scalar and vector couplings to gluons

A bstract We use on-shell methods to calculate tree-level effective field theory (EFT) amplitudes, with no reference to the EFT operators. Lorentz symmetry, unitarity and Bose statistics determine the allowed kinematical structures. As a by-product, the number of independent EFT operators simply fol...

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Published inThe journal of high energy physics Vol. 2019; no. 2; pp. 1 - 26
Main Authors Shadmi, Yael, Weiss, Yaniv
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer Berlin Heidelberg 01.02.2019
Springer Nature B.V
SpringerOpen
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Summary:A bstract We use on-shell methods to calculate tree-level effective field theory (EFT) amplitudes, with no reference to the EFT operators. Lorentz symmetry, unitarity and Bose statistics determine the allowed kinematical structures. As a by-product, the number of independent EFT operators simply follows from the set of polynomials in the Mandelstam invariants, subject to kinematical constraints. We demonstrate this approach by calculating several amplitudes with a massive, SM-singlet, scalar ( h ) or vector ( Z ′ ) particle coupled to gluons. Specifically, we calculate hggg , hhgg and Z ′ ggg amplitudes, which are relevant for the LHC production and three-gluon decays of the massive particle. We then use the results to derive the massless- Z ′ amplitudes, and show how the massive amplitudes decompose into the massless-vector plus scalar amplitudes. Amplitudes with the gluons replaced by photons are straightforwardly obtained from the above.
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ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP02(2019)165