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 in | The journal of high energy physics Vol. 2019; no. 2; pp. 1 - 26 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
01.02.2019
Springer Nature B.V SpringerOpen |
Subjects | |
Online Access | Get full text |
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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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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP02(2019)165 |