30 research outputs found

    Constraints on the two-Higgs-doublet model

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    The two-Higgs-doublet model provides a simple, yet interesting, generalization of the SM Higgs sector. We study the CP-conserving version of this model with general, flavor-diagonal, Yukawa couplings. Indirect constraints are obtained from flavor physics on the charged Higgs boson mass and couplings. The relation of these bounds to those for the more specialized two-Higgs-doublet model types with a Z2Z_2 symmetry is discussed.Comment: 4 pages, 3 figures. Talk given at SUSY09, Boston (MA), June 200

    Improved prediction for the mass of the W boson in the NMSSM

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    Electroweak precision observables, being highly sensitive to loop contributions of new physics, provide a powerful tool to test the theory and to discriminate between different models of the underlying physics. In that context, the WW boson mass, MWM_W, plays a crucial role. The accuracy of the MWM_W measurement has been significantly improved over the last years, and further improvement of the experimental accuracy is expected from future LHC measurements. In order to fully exploit the precise experimental determination, an accurate theoretical prediction for MWM_W in the Standard Model (SM) and extensions of it is of central importance. We present the currently most accurate prediction for the WW boson mass in the Next-to-Minimal Supersymmetric extension of the Standard Model (NMSSM), including the full one-loop result and all available higher-order corrections of SM and SUSY type. The evaluation of MWM_W is performed in a flexible framework, which facilitates the extension to other models beyond the SM. We show numerical results for the WW boson mass in the NMSSM, focussing on phenomenologically interesting scenarios, in which the Higgs signal can be interpreted as the lightest or second lightest CP-even Higgs boson of the NMSSM. We find that, for both Higgs signal interpretations, the NMSSM MWM_W prediction is well compatible with the measurement. We study the SUSY contributions to MWM_W in detail and investigate in particular the genuine NMSSM effects from the Higgs and neutralino sectors.Comment: 43 pages, 21 figure

    Prospects for GMRT to Observe Radio Waves from UHE Particles Interacting with the Moon

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    Ultra high energy (UHE) particles of cosmic origin impact the lunar regolith and produce radio signals through Askaryan effect, signals that can be detected by Earth based radio telescopes. We calculate the expected sensitivity for observation of such events at the Giant Metrewave Radio Telescope (GMRT), both for UHE cosmic rays (CR) and UHE neutrino interactions. We find that for 30 days of observation time a significant number of detectable events is expected above 102010^{20} eV for UHECR or neutrino fluxes close to the current limits. Null detection over a period of 30 days will lower the experimental bounds on UHE particle fluxes by magnitudes competitive to both present and future experiments at the very highest energies.Comment: 21 pages, 9 figure

    New angles on top quark decay to a charged Higgs

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    To properly discover a charged Higgs Boson (H±H^\pm) requires its spin and couplings to be determined. We investigate how to utilize \ttbar spin correlations to analyze the H±H^\pm couplings in the decay tbH+bτ+ντt\to bH^+\to b\tau^+\nu_\tau. Within the framework of a general Two-Higgs-Doublet Model, we obtain results on the spin analyzing coefficients for this decay and study in detail its spin phenomenology, focusing on the limits of large and small values for tanβ\tan\beta. Using a Monte Carlo approach to simulate full hadron-level events, we evaluate systematically how the H±τ±ντH^\pm\to\tau^\pm\nu_\tau decay mode can be used for spin analysis. The most promising observables are obtained from azimuthal angle correlations in the transverse rest frames of t(tˉ)t(\bar{t}). This method is particularly useful for determining the coupling structure of H±H^\pm in the large tanβ\tan\beta limit, where differences from the SM are most significant.Comment: 28 pages, 13 figures. Uses JHEP forma
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