32,647 research outputs found

    Decay of Z into Three Pseudoscalar Bosons

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    We consider the decay of the ZZ boson into three pseudoscalar bosons in a general two-Higgs-doublet model. Assuming mAm_A to be very small, and that of the two physical neutral scalar bosons h1h_1 and h2h_2, AA only couples to ZZ through h1h_1, we find the ZAAAZ \to A A A branching fraction to be negligible for moderate values of tanβv2/v1\tan \beta \equiv v_2/v_1, if there is no λ5(Φ1Φ2)2+h.c.\lambda_5 (\Phi_1^\dagger \Phi_2)^2 + h.c. term in the Higgs potential; otherwise there is no absolute bound but very large quartic couplings (beyond the validity of perturbation theory) are needed for it to be observable.Comment: 8 pages including 1 fi

    Lower Bound on the Pseudoscalar Mass in the Minimal Supersymmetric Standard Model

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    In the Higgs sector of the Minimal Supersymmetric Standard Model, the mass of the pseudoscalar AA is an independent parameter together with tanβv2/v1\tan \beta \equiv v_2/v_1. If mAm_A is small, then the process e+eh+Ae^+ e^- \to h + A is kinematically allowed and is suppressed only if tanβ\tan \beta is small. On the other hand, the mass of the charged Higgs boson is now near MWM_W, and the decay tb+h+t \to b + h^+ is enhanced if tanβ\tan \beta is small. Since the former has not been observed, and the branching fraction of tb+Wt \to b + W cannot be too small (by comparing the experimentally derived ttˉt \bar t cross section from the leptonic channels with the theoretical prediction), we can infer a phenomenological lower bound on mAm_A of at least 60 GeV for all values of tanβ\tan \beta.Comment: 11 pages including 2 figs, reference adde

    Higgs and Z-boson Signatures of Supersymmetry

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    In supersymmetric theories of nature the Higgsino fermionic superpartner of the Higgs boson can arise as the lightest standard model superpartner depending on the couplings between the Higgs and supersymmetry breaking sectors. In this letter the production and decay of Higgsino pairs to the Goldstone fermion of supersymmetry breaking and the Higgs boson, h, or gauge bosons, Z or γ\gamma are considered. Relatively clean di-boson final states, hh, hγh \gamma, hZ, ZγZ \gamma, or ZZ, with a large amount of missing energy result. The latter channels provide novel discovery modes for supersymmetry at high energy colliders since events with Z bosons are generally rejected in supersymmetry searches. In addition, final states with real Higgs bosons can potentially provide efficient channels to discover and study a Higgs signal at the Fermilab Tevatron Run II.Comment: 11 pages, LaTeX, 3 figure
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