Coupling WW, ZZ unitarized amplitudes to $$\gamma \gamma $$ γ γ in the TeV region

Abstract We define and calculate helicity partial-wave amplitudes for processes linking the Electroweak Symmetry Breaking Sector (EWSBS) to $$\gamma \gamma $$ γ γ , employing (to NLO) the Higgs-EFT (HEFT) extension of the Standard Model and the Equivalence Theorem, while neglecting all particle mass...

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Bibliographic Details
Main Authors: Rafael L. Delgado, Antonio Dobado, Felipe J. Llanes-Estrada
Format: Article
Language:English
Published: SpringerOpen 2017-03-01
Series:European Physical Journal C: Particles and Fields
Subjects:
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-4768-y
Description
Summary:Abstract We define and calculate helicity partial-wave amplitudes for processes linking the Electroweak Symmetry Breaking Sector (EWSBS) to $$\gamma \gamma $$ γ γ , employing (to NLO) the Higgs-EFT (HEFT) extension of the Standard Model and the Equivalence Theorem, while neglecting all particle masses. The resulting amplitudes can be useful in the energy regime ( $$500~\mathrm{{GeV}}{-}3~\mathrm{{TeV}}$$ 500 GeV - 3 TeV ). We also deal with their unitarization so that resonances of the EWSBS can simultaneously be described in the $$\gamma \gamma $$ γ γ initial or final states. Our resulting amplitudes satisfy unitarity, perturbatively in $$\alpha $$ α , but for all s values. In this way we improve on the HEFT that fails as interactions become stronger with growing s and we provide a natural framework for the decay of dynamically generated resonances into WW, ZZ and $$\gamma \gamma $$ γ γ pairs.
ISSN:1434-6044
1434-6052