Searches for New Physics in the Standard Model's Electroweak Sector: Quartic Anomalous Couplings with Vector Boson Fusion and Flavor Changed Neutral Current in the SU(3)C⊗SU(3)L⊗U(1)XSU(3)_{C}\otimes SU(3)_{L}\otimes U(1)_{X} model

preprint2013arXivOpen access

Abstract

In this thesis we investigated, at partonic level and leading order, the LHC potencial operating with s=14\sqrt{s}=14 TeV and integrated luminosity of L=100  fb−1L=100\;{fb}^{-1} to probe "pure" (without triple vertex contributions) anomalous electroweak quartic couplings, WWWWWWWW and WWZZWWZZ, in the semileptonic pp→l±νljjjjpp \rightarrow l^{\pm}ν_{l}jjjj channel, enhanced by the Vector Boson Fusion collider signatures. Deviations on SM quartic couplings were parameterized in a model independent approach, realized linearly (LS0L_{S0} and LS1L_{S1} operators) or not (L4L_{4} and L5L_{5} operators), on the basis of effective lagrangians. Being our analysis essentially events counting-and-cut based, we took into account all possible backgrounds (irreducible, QCD and top quarks processes) considered at O(αem6){\cal O}(α_{em}^{6}), ${\cal O(α_{em}^{4}α_{s}^{2})$ and O(αem2αs4){\cal O}(α_{em}^{2}α_{s}^{4}). In this way, we have obtained the following constraints for the non-linear α4α_{4} and α5α_{5} anomalous couplings: ∣α4,5∣≲0.01|α_{4,5}| \lesssim 0.01 to 0.02 at 3σσ. Based on non-linear results, we have estimated, for a specific choice of factorization and renormalization scale, the linear parameters f0f_{0} and f1f_{1} constraints as −22≤f0Λ4  (TeV−4)≤20,and−26≤f1Λ4  (TeV−4)≤24-22 \leq \dfrac{f_{0}}{Λ^{4}}\;({TeV}^{-4}) \leq 20, \quad {and} \quad -26 \leq \dfrac{f_{1}}{Λ^{4}}\;({TeV}^{-4}) \leq 24 at 3σσ. On a different approach, manipulating one extension of the SM named 331RHN331_{RHN}, we have evaluated the contribution of new sources of FCNC for the difference of mass of neutral meson systems, K0−K0ˉK_{0}-\bar{K_{0}}, D0−D0ˉD^{0}-\bar{D^0} and Bd0−Bd0ˉB^0_d-\bar{B^0_d}. Bounds related to these systems may be significantly strengthened in the presence of these new interactions allowing stronger constraints on the parameter space of the model.

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