Abstract

In this paper, we explore the potential of the LHC to measure the rate of pp → p WWγ p process, also to probe the new effective couplings contributing to the WWγ and WWγγ vertices. The analysis is performed at the sqrt{s} = 13 TeV, in the dileptonic decay channel, and assuming 300 fb−1 integrated luminosity (IL). In addition to the presence of two opposite sign leptons, a photon, and missing energy, the distinctive signature of this process is the presence of two intact protons flying few millimeters from the initial beam direction in both sides of interaction points which suppress the background process effectively. To exploit this feature of signal we benefit from forward detectors (FDs) placed about 200 meters from the interaction point to register the kinematics of tagged protons. In order to overcome the major sources of backgrounds, we introduced three categories of selection cuts dealing with objects that strike the central detector, protons hitting the FDs, and correlations of central objects and protons, respectively. We also evaluate the probability of pile-up protons to be tagged in the FDs as a function of the mean number of pile-up. Then the sensitivity of the LHC to observe this process and constraints on multi-boson effective couplings are extracted. The obtained expected limits show very good improvements for dimension-8 quartic couplings and competitive bounds on dimension-6 anomalous triple couplings w.r.t. the current experimental limits. Therefore, we propose this process to the LHC experiments as a sensitive and complementary channel to study the multi-gauge boson couplings.

Highlights

  • Gauge bosons or lead to new vertices both known as anomalous couplings [1]

  • In this paper, we explore the potential of the LHC to measure the rate of pp → pWWγp process, to probe the new effective coupl√ings contributing to the W W γ and W W γγ vertices

  • Depending on the flavor of leptons decayed from W boson, we divide our signal region into the same flavor leptonic (SF) channel consists of e+e−, μ+μ− events and different flavor (DF) channel e+μ−, e−μ+, because the SF channel suffers from a large contribution of l+l−γ background process while DF does not

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Summary

Photon-photon interaction at the LHC

Photon-photon interactions at the LHC can be studied through the CEP that is defined as pp → p ⊕ X ⊕ p. Measurement of the forward protons permits to predict the kinematics of centrally produced state and matching them can lead to several orders of magnitude suppression in the background processes. Benefiting from these properties which FDs granted us, the CEP could provide a rich testing ground for electroweak and QCD sector of the SM and unique window to physics beyond the SM. Where dLγγ dWmiss is the two photons luminosity spectrum which can be obtained by integrating the product of two photon rates f (Eγ1)f (Eγ2) over the energy of photons while the two p√hotons invariant mass or equivalently total missing mass of protons Wmiss = 2 Eγ1Eγ2 = √ξ1ξ2s remains fix.

EFT for anomalous gauge couplings involving photon
WWγ production in γγ collisions
Analysis design
Selection cuts
Pile-up implementation
Inclusive backgrounds with pile-up protons
Double pomeron exchange processes
Sensitivity to anomalous gauge boson couplings
Statistical method
Triple gauge boson couplings
Quartic gauge boson couplings
Summary and remarks
Full Text
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