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    Irrotational dust with Div H=0

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    For irrotational dust the shear tensor is consistently diagonalizable with its covariant time derivative: σab=0=σ˙ab,  ab\sigma_{ab}=0=\dot{\sigma}_{ab},\; a\neq b, if and only if the divergence of the magnetic part of the Weyl tensor vanishes: div H=0div~H = 0. We show here that in that case, the consistency of the Ricci constraints requires that the magnetic part of the Weyl tensor itself vanishes: Hab=0H_{ab}=0.Comment: 19 pages. Latex. Also avaliable at http://shiva.mth.uct.ac.za/preprints/text/lesame2.te

    Exotic Higgs Decay via Charged Higgs

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    The most common search channel for heavy neutral Higgses in models with an extension of the Standard Model Higgs sector is A/H0ττA/H^0\rightarrow \tau\tau, which becomes ineffective when new decay modes of A/H0A/H^0 open. In this paper, we analyzed two such channels involving charged Higgses in the final states: A/H0W±HA/H^0 \rightarrow W^\pm H^\mp and H0H+HH^0 \rightarrow H^+H^-. With the consequent decay of H±τνH^\pm\rightarrow \tau\nu, we found that the limits for σ×BR(ggA/H0W±H)×BR(H±τν)\sigma\times{BR}(gg \rightarrow A/H^0 \rightarrow W^\pm H^\mp)\times {BR}(H^\pm \rightarrow \tau \nu) vary from 30 to 10 fb for mA/H0m_{A/H^0} between 300 and 1000 GeV for 95% C.L. exclusion, and about 80 to 30 fb for 5σ\sigma discovery. For H+HH^+H^- mode, 95% C.L. limits on σ×BR(ggH0H+H)×BR2(H±τν)\sigma\times {BR}(gg\to H^0\to H^+ H^-)\times {BR}^2(H^\pm\to \tau\nu) vary from 9 to 4 fb for mH0m_{H^0} between 400 and 1000 GeV, while the 5σ\sigma reach is about 20 to 10 fb. We further interpret the cross section limits in the Type II 2HDM parameter space. While AW±HA\rightarrow W^\pm H^\mp offers great sensitivity in both sin(βα)\sin(\beta-\alpha) versus tanβ\tan\beta and mAm_A versus tanβ\tan\beta parameter space, H0H+HH^0\rightarrow H^+ H^- can cover most of the parameter space for H0H^0. Reach in H0W±HH^0\rightarrow W^\pm H^\mp is more limited, especially for mH0>2mH±m_{H^0}>2 m_{H^\pm}. It is, however, complementary to H0H+HH^0\rightarrow H^+ H^- when BR(H0H+H){BR}(H^0\rightarrow H^+ H^-) is accidentally suppressed.Comment: 19 pages, 11 figures, version appear in JHE

    Higgs-photon resonances

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    We study models that produce a Higgs boson plus photon (h0γh^0 \gamma) resonance at the LHC. When the resonance is a ZZ' boson, decays to h0γh^0 \gamma occur at one loop. If the ZZ' boson couples at tree-level to quarks, then the h0γh^0 \gamma branching fraction is typically of order 10510^{-5} or smaller. Nevertheless, there are models that would allow the observation of Zh0γZ' \to h^0 \gamma at s=13\sqrt{s} = 13 TeV with a cross section times branching fraction larger than 1 fb for a ZZ' mass in the 200--450 GeV range, and larger than 0.1 fb for a mass up to 800 GeV. The 1-loop decay of the ZZ' into lepton pairs competes with h0γh^0 \gamma, even if the ZZ' couplings to leptons vanish at tree level. We also present a model in which a ZZ' boson decays into a Higgs boson and a pair of collimated photons, mimicking an h0γh^0 \gamma resonance. In this model, the h0γh^0 \gamma resonance search would be the discovery mode for a ZZ' as heavy as 2 TeV. When the resonance is a scalar, although decay to h0γh^0 \gamma is forbidden by angular momentum conservation, the h0h^0 plus collimated photons channel is allowed. We comment on prospects of observing an h0γh^0 \gamma resonance through different Higgs decays, on constraints from related searches, and on models where h0h^0 is replaced by a nonstandard Higgs boson.Comment: 22 page

    chi_cJ Decays to h^+h^-h^0

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    Using a sample of 3x10^6 psi(2S) decays recorded by the CLEO detector, we study three body decays of the chi_{c0}, chi_{c1}, and chi_{c2} produced in radiative decays of the psi(2S). We consider the decay modes pi+ pi- eta, K+ K- eta, p pbar eta, pi+ pi- etaprime, K+ K- pi0, p pbar pi0, pi+ K- K0S, and K+ pbar Lambda measuring branching fractions or placing upper limits. For chi_{c1} to pi+ pi- eta, K+ K- pi0, and pi+ K- K0S our observed samples are large enough to study the substructure in a Dalitz plot analysis. The results presented in this document are preliminary.Comment: 22 pages postscript,also available through http://www.lepp.cornell.edu/public/CONF/2006, Contributed to ICHEP0
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