We discuss how to perform consistent extractions of anomalous triple gauge couplings (aTGC) from electroweak boson pair production at the LHC in the Standard Model Effective Field Theory (SMEFT). After recasting recent ATLAS and CMS searches in pp -> W Z (WW) -> l(1)vl(+)l(-)(v(l)) channels, we find that: (a) working consistently at order Lambda(-2) in the SMEFT expansion the existing aTGC bounds from Higgs and LEP-2 data are not improved, (b) the strong limits quoted by the experimental collaborations are due to the partial Lambda(-4) corrections (dimension-6 squared contributions). Using helicity selection rule arguments we are able to explain the suppression in some of the interference terms, and discuss conditions on New Physics (NP) models that can benefit from such LHC analyses. Furthermore, standard analyses assume implicitly a quite large NP scale, an assumption that can be relaxed by imposing cuts on the underlying scale of the process (root s). In practice, we find almost no correlation between root s and the experimentally accessible quantities, which complicates the SMEFT interpretation. Nevertheless, we provide a method to set (conservative) aTGC bounds in this situation, and recast the present searches accordingly. Finally, we introduce a simple NP model for aTGC to compare the bounds obtained directly in the model with those from the SMEFT analysis.

Anomalous triple gauge couplings in the effective field theory approach at the LHC / Falkowski, Adam; Gonzalez-Alonso, Martin; Greljo, Admir; Marzocca, David; Son, Minho. - In: JOURNAL OF HIGH ENERGY PHYSICS. - ISSN 1029-8479. - 2017:2(2017), pp. 1-31. [10.1007/jhep02(2017)115]

Anomalous triple gauge couplings in the effective field theory approach at the LHC

Adam Falkowski;Admir Greljo;David Marzocca;Minho Son
2017-01-01

Abstract

We discuss how to perform consistent extractions of anomalous triple gauge couplings (aTGC) from electroweak boson pair production at the LHC in the Standard Model Effective Field Theory (SMEFT). After recasting recent ATLAS and CMS searches in pp -> W Z (WW) -> l(1)vl(+)l(-)(v(l)) channels, we find that: (a) working consistently at order Lambda(-2) in the SMEFT expansion the existing aTGC bounds from Higgs and LEP-2 data are not improved, (b) the strong limits quoted by the experimental collaborations are due to the partial Lambda(-4) corrections (dimension-6 squared contributions). Using helicity selection rule arguments we are able to explain the suppression in some of the interference terms, and discuss conditions on New Physics (NP) models that can benefit from such LHC analyses. Furthermore, standard analyses assume implicitly a quite large NP scale, an assumption that can be relaxed by imposing cuts on the underlying scale of the process (root s). In practice, we find almost no correlation between root s and the experimentally accessible quantities, which complicates the SMEFT interpretation. Nevertheless, we provide a method to set (conservative) aTGC bounds in this situation, and recast the present searches accordingly. Finally, we introduce a simple NP model for aTGC to compare the bounds obtained directly in the model with those from the SMEFT analysis.
2017
2017
2
1
31
115
10.1007/jhep02(2017)115
https://arxiv.org/abs/1609.06312
Falkowski, Adam; Gonzalez-Alonso, Martin; Greljo, Admir; Marzocca, David; Son, Minho
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.11767/132022
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