35,047 research outputs found

    Highlights of Supersymmetric Hypercharge ±1\pm1 Triplets

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    The discovery of a standard model (SM)-like Higgs boson with a relatively heavy mass mhm_h and hints of di-photon excess has deep implication to supersymmetric standard models (SSMs). We consider the SSM extended with hypercharge ±1\pm1 triplets, and investigate two scenarios of it: (A) Triplets significantly couple to the Higgs doublets, which can substantially raise mhm_h and simultaneously enhance the Higgs to di-photon rate via light chargino loops; (B) Oppositely, these couplings are quite weak and thus mhm_h can not be raised. But the doubly-charged Higgs bosons, owing to the gauge group structure, naturally interprets why there is an excess rather than a deficient of Higgs to di-photon rate. Additionally, the pseudo Dirac triplet fermion is an inelastic non-thermal dark matter candidate. Light doubly-charged particles, especially the doubly-charged Higgs boson around 100 GeV in scenario B, are predicted. We give a preliminary discussion on their search at the LHC.Comment: JHEP version. Typos fixed, comments, references and acknowledge adde

    Light Doubly Charged Higgs Boson via the WW∗WW^* Channel at LHC

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    The doubly charged Higgs bosons H±±H^{\pm\pm} searches at the Large Hadron Collider (LHC) have been studied extensively and strong bound is available for H±±H^{\pm\pm} dominantly decaying into a pair of same-sign di-leptons. In this paper we point out that there is a large cavity in the light H±±H^{\pm\pm} mass region left unexcluded. In particular, H±±H^{\pm\pm} can dominantly decay into WWWW or WW∗WW^* (For instance, in the type-II seesaw mechanism the triplet acquires a vacuum expectation value around 1 GeV.), and then it is found that H±±H^{\pm\pm} with mass even below 2mW2m_W remains untouched by the current collider searches. Searching for such a H±±H^{\pm\pm} at the LHC is the topic of this paper. We perform detailed signal and background simulation, especially including the non-prompt ttˉt\bar{t} background which is the dominant one nevertheless ignored before. We show that such H±±H^{\pm\pm} should be observable at the 14 TeV LHC with 10-30 fb−1^{-1} integrated luminosity.Comment: 23 pages, 4 figures, typos fixed, references added, EPJC versio
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