Search for anomalous quartic ZZγγZZγγ couplings in photon-photon collisions

preprint2016arXivOpen access

Abstract

The self-couplings of the electroweak gauge bosons are completely specified by the non-Abelian gauge nature of the Standard Model (SM). The direct study of these couplings provides a significant opportunity to test the validity of the SM and the existence of new physics beyond the SM up to the high energy scale. For this reason, we investigate the potential of the processes γγ→ZZγγ\rightarrow ZZ, e−γ→e−γ∗γ→e−Z Ze^{-}γ\rightarrow e^{-}γ^{*}γ\rightarrow e^{-}Z\, Z and e+e−→e+γ∗γ∗e−→e+ Z Z e−e^{+}e^{-} \rightarrow e^{+}γ^{*} γ^{*} e^{-} \rightarrow e^{+}\, Z\, Z\, e^{-} to examine the anomalous quartic couplings of ZZγγZZγγ vertex at the Compact Linear Collider (CLIC) with center-of-mass energy 33 TeV. We calculate 95%95\% confidence level sensitivities on the dimension-8 parameters with various values of the integrated luminosity. We show that the best bounds on the anomalous fM2Λ4\frac{f_{M2}}{Λ^{4}}, fM3Λ4\frac{f_{M3}}{Λ^{4}}, fT0Λ4\frac{f_{T0}}{Λ^4} and fT9Λ4\frac{f_{T9}}{Λ^4} couplings arise from γγ→ZZγγ\rightarrow ZZ process among those three processes at center-of-mass energy of 3 TeV and integrated luminosity of Lint=2000L_{int}=2000 fb−1^{-1} are found to be [−3.30;3.30]×10−3[-3.30;3.30]\times 10 ^{-3} TeV−4^{-4}, [−1.20;1.20]×10−2[-1.20;1.20]\times 10 ^{-2} TeV−4^{-4}, [−3.40;3.40]×10−3[-3.40;3.40]\times 10 ^{-3} TeV−4^{-4} and [−1.80;1.80]×10−3[-1.80;1.80]\times 10 ^{-3} TeV−4^{-4}, respectively.

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