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通过WZ散射在LHC上产生矢量共振:一个么正化的EChL分析

Production of vector resonances at the LHC via WZ-scattering: a unitarized EChL analysis

R. L. Delgado, A. Dobado, D. Espriu, C. Garcia-Garcia, M. J. Herrero, X. Marcano, J. J. Sanz-Cillero

摘要:

在目前的工作中,我们研究的矢量玻色子散射$WZ \to WZ$在LHC的矢量共振的生产,并探讨这些共振的预期未来LHC亮度的敏感性。我们假设这些矢量共振是从纵向规范玻色子,$W_L$和$Z_L$的自相互作用动态产生的,并在电弱手征拉格朗日的框架下工作,以模型独立的方式描述这些模式的假定强动力学。用反振幅方法导出了矢量共振、质量、宽度以及与$W$和$Z$规范玻色子的耦合性质。我们实现所有这些功能到一个单一的模型,IAM-MC,适用于蒙特卡洛,内置在一个拉格朗日语言的电弱手征拉格朗日和手征拉格朗日矢量共振,模仿IAM的共振行为,并提供单一的振幅。该模型已在MadGraph中实现,使我们能够对LHC的信号与背景事件进行现实的研究。特别是,我们把我们的研究集中在$pp\to WZjj$类型的事件,讨论的最后$WZ$的强子和半轻子通道的潜力,下一步更详细地探索最清晰的信号。这些都是由规范玻色子的轻子衰变提供的,导致了具有$\ell_1^+\ell_1^-\ell_2^+νjj$的终态,$\ell=e,μ$,具有非常独特的签名,并清楚地显示出与质量在1.5-2.5 TeV范围内的共振的出现,我们已经探索过了。

英文摘要:

In the present work we study the production of vector resonances at the LHC by means of the vector boson scattering $WZ \to WZ$ and explore the sensitivities to these resonances for the expected future LHC luminosities. We are assuming that these vector resonances are generated dynamically from the self interactions of the longitudinal gauge bosons, $W_L$ and $Z_L$, and work under the framework of the electroweak chiral Lagrangian to describe in a model independent way the supposedly strong dynamics of these modes. The properties of the vector resonances, mass, width and couplings to the $W$ and $Z$ gauge bosons are derived from the inverse amplitude method approach. We implement all these features into a single model, the IAM-MC, adapted for MonteCarlo, built in a Lagrangian language in terms of the electroweak chiral Lagrangian and a chiral Lagrangian for the vector resonances, which mimics the resonant behavior of the IAM and provides unitary amplitudes. The model has been implemented in MadGraph, allowing us to perform a realistic study of the signal versus background events at the LHC. In particular, we have focused our study on the $pp\to WZjj$ type of events, discussing first on the potential of the hadronic and semileptonic channels of the final $WZ$, and next exploring in more detail the clearest signals. These are provided by the leptonic decays of the gauge bosons, leading to a final state with $\ell_1^+\ell_1^-\ell_2^+νjj$, $\ell=e,μ$, having a very distinctive signature, and showing clearly the emergence of the resonances with masses in the range of 1.5-2.5 TeV, which we have explored.

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