Our aim is to establish some signatures of the extra gauge boson Z ′ , predicted in two versions ... more Our aim is to establish some signatures of the extra gauge boson Z ′ , predicted in two versions of SU (3) C × SU (3) L × U (1) X model and to show possible differences between these signatures. First, by considering the process e + + e − −→ µ + + µ − , we obtain some observables and next, by considering additional hadronic final states, we obtain lower bounds for M Z ′ , within 95% C.L.. We also include our preliminary results concerning pp and pp collisions in order to support our conclusions about the possibility to discriminate the various versions of 3-3-1 model. From our analysis we conclude that linear colliders can show a clear signature for the existence of Z ′ predicted in the 3-3-1 model and also that it can discriminate the versions.
Our aim is to establish some signatures of the extra gauge boson Z ′ , predicted in two versions ... more Our aim is to establish some signatures of the extra gauge boson Z ′ , predicted in two versions of SU (3) C × SU (3) L × U (1) X model and to show possible differences between these signatures. First, by considering the process e + + e − −→ µ + + µ − , we obtain some observables and next, by considering additional hadronic final states, we obtain lower bounds for M Z ′ , within 95% C.L.. We also include our preliminary results concerning pp and pp collisions in order to support our conclusions about the possibility to discriminate the various versions of 3-3-1 model. From our analysis we conclude that linear colliders can show a clear signature for the existence of Z ′ predicted in the 3-3-1 model and also that it can discriminate the versions.
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Papers by Giovanna Prado