9,211 research outputs found

    LHC Phenomenology of Type II Seesaw: Nondegenerate Case

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    In this paper, we thoroughly investigate the LHC phenomenology of the type II seesaw mechanism for neutrino masses in the nondegenerate case where the triplet scalars of various charge (H±±,H±,H0,A0H^{\pm\pm}, H^\pm, H^0, A^0) have different masses. Compared with the degenerate case, the cascade decays of scalars lead to many new, interesting signal channels. In the positive scenario where MH±±<MH±<MH0/A0M_{H^{\pm\pm}}<M_{H^\pm}<M_{H^0/A^0}, the four-lepton signal is still the most promising discovery channel for the doubly-charged scalars H±±H^{\pm\pm}. The five-lepton signal is crucial to probe the mass spectrum of the scalars, for which, for example, a 5σ5\sigma reach at 14 TeV LHC for MH±=430GeVM_{H^{\pm}}=430 GeV with MH±±=400GeVM_{H^{\pm\pm}}=400 GeV requires an integrated luminosity of 76/fb. And the six-lepton signal can be used to probe the neutral scalars H0/A0H^0/A^0, which are usually hard to detect in the degenerate case. In the negative scenario where MH±±>MH±>MH0/A0M_{H^{\pm\pm}}>M_{H^\pm}>M_{H^0/A^0}, the detection of H±±H^{\pm\pm} is more challenging, when the cascade decay H±±→H±W±∗H^{\pm\pm}\to H^{\pm}W^{\pm*} is dominant. The most important channel is the associated H±H0/A0H^{\pm}H^0/A^0 production in the final state ℓ±ETbbˉbbˉ\ell^\pm\cancel{E}_Tb\bar{b}b\bar{b}, which requires a luminosity of 109/fb for a 5σ5\sigma discovery, while the final state ℓ±ETbbˉτ+τ−\ell^\pm\cancel{E}_Tb\bar{b}\tau^+\tau^- is less promising. Moreover, the associated H0A0H^0A^0 production can give same signals as the standard model Higgs pair production. With a much larger cross section, the H0A0H^0A^0 production in the final state bbˉτ+τ−b\bar{b}\tau^+\tau^- could reach 3σ3\sigma significance at 14 TeV LHC with a luminosity of 300/fb. In summary, with an integrated luminosity of order 500/fb, the triplet scalars can be fully reconstructed at 14 TeV LHC in the negative scenario.Comment: 41 pages, 20 figures, 7 tables. Version 2 accepted by PRD. 41 pages, 18 figures. Main changes are, (1) rewording in secs III and IV, removing 2 figs and quoting ref [34]; (2) a paragraph added before eq (10) to clarify constraints from electroweak precision data; (3) a paper added to ref [11]. No changes in result

    LHC Phenomenology of the Type II Seesaw Mechanism: Observability of Neutral Scalars in the Nondegenerate Case

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    This is a sequel to our previous work on LHC phenomenology of the type II seesaw model in the nondegenerate case. In this work, we further study the pair and associated production of the neutral scalars H^0/A^0. We restrict ourselves to the so-called negative scenario characterized by the mass order M_{H^{\pm\pm}}>M_{H^\pm}>M_{H^0/A^0}, in which the H^0/A^0 production receives significant enhancement from cascade decays of the charged scalars H^{\pm\pm},~H^\pm. We consider three important signal channels---b\bar{b}\gamma\gamma, b\bar{b}\tau^+\tau^-, bbˉℓ+ℓ−ETb\bar{b}\ell^+\ell^-\cancel{E}_T---and perform detailed simulations. We find that at the 14 TeV LHC with an integrated luminosity of 3000/fb, a 5\sigma mass reach of 151, 150, and 180 GeV, respectively, is possible in the three channels from the pure Drell-Yan H^0A^0 production, while the cascade-decay-enhanced H^0/A^0 production can push the mass limit further to 164, 177, and 200 GeV. The neutral scalars in the negative scenario are thus accessible at LHC run II.Comment: v1: 32 pages, 17 figures, 3 tables. v2: added 2 refs (2nd in [61] and [66]), revised Acknowledgments, and corrected grammatical errors according to proofs; no other change
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