Search for anomalous quartic WWZγWWZγ couplings at the future linear e+e−e^{+}e^{-} collider

preprint2015arXivOpen access

Abstract

In this paper, the potentials of two different processes e+e−→W−W+γe^{+}e^{-}\rightarrow W^{-} W^{+}γ and e+e−→e+γ∗e−→e+W−Zνee^{+}e^{-} \rightarrow e^{+}γ^{*} e^{-} \rightarrow e^{+} W^{-} Z ν_{e} at the Compact Linear Collider (CLIC) are examined to probe the anomalous quartic WWZγWWZγ gauge couplings. For s=0.5,1.5\sqrt{s}=0.5, 1.5 and 3 TeV energies at the CLIC, 95%95\% confidence level limits on the anomalous coupling parameters defining the dimension-six operators are found via the effective Lagrangian approach in a model independent way. The best limits on the anomalous couplings k0WΛ2\frac{k_{0}^{W}}{Λ^{2}}, kcWΛ2\frac{k_{c}^{W}}{Λ^{2}}, k2mΛ2\frac{k_{2}^{m}}{Λ^{2}} and anΛ2\frac{a_{n}}{Λ^{2}} which can be achieved with the integrated luminosity of Lint=590L_{int}=590 fb−1^{-1} at the CLIC with s=3\sqrt{s}=3 TeV are [−8.80; 8.73]×10−8[-8.80;\, 8.73]\times 10^{-8} GeV−2^{-2}, [−1.53; 1.51]×10−7[-1.53; \, 1.51]\times 10^{-7} GeV−2^{-2}, [−3.75; 3.74]×10−7[-3.75; \, 3.74]\times 10^{-7} GeV−2^{-2} and [−9.13; 9.09]×10−7[-9.13;\,9.09]\times 10^{-7} GeV−2^{-2}, respectively.

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