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The Hidden Abelian Higgs Model (HAHM) is an extension of the Standard Modelbased on the gauge group $G =SU(3)_{C} \times SU(2)_{L} \times U(1)_{Y} \timesU(1)_{X}$ i.e. an extra $U(1)_{X}$ gauge group in addition to the SM gaugegroups.In HAHM, an Abelian Hidden sector is coupled to the SM, and theresulting new Higgs boson H and new neutral gauge boson $Z_{HAHM}$ fields areallowed to mix with the corresponding SM fields. In this work, we search forthe new neutral gauge boson $Z_{HAHM}$ and new Higgs boson in the context ofthe Hidden Abelian Higgs Model (HAHM) through the decay process$pp(\bar{p})\rightarrow H\rightarrow Z_{HAHM}Z_{HAHM}\rightarrow\textit{l}^{\pm}\textit{l}^{\mp}\textit{l}^{\pm}\textit{l}^{\mp},(\textit{l}=e,\mu)$with 4 charged leptons in the final state in the mass range $200\leq Z_{HAHM}\leq 700$ GeV and the production and decay of new Higgs boson with 2 chargedleptons in the final state of the process $pp(\bar{p})\rightarrowH\rightarrow\textit{l}^{\pm}\textit{l}^{\mp}jj ,(\textit{l}=e,\mu)$ with jetsor final state of the proces $pp(\bar{p})\rightarrow H\rightarrow\textit{l}^{\pm}\textit{l}^{mp}\nu\bar{\nu},(l=e,\mu)$ with missing energy.Weused Monte Carlo data produced from proton-proton collisions at the LHC CERN(CMS and ATLAS detectors) for different center of mass energies up to$\sqrt{s}= 14 TeV$

Phenomenology of Hidden Abelian Higgs Model at Hadron Colliders using  Neural Networks and Monte Carlo Techniques (Gauge Sector $Z_{HAHM}$ & Scalar  Sector H)