9,478 research outputs found

    The Effect of Composite Resonances on Higgs decay into two photons

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    In scenarios of strongly coupled electroweak symmetry breaking, heavy composite particles of different spin and parity may arise and cause observable effects on signals that appear at loop levels. The recently observed process of Higgs to γγ\gamma \gamma at the LHC is one of such signals. We study the new constraints that are imposed on composite models from HγγH\to \gamma\gamma, together with the existing constraints from the high precision electroweak tests. We use an effective chiral Lagrangian to describe the effective theory that contains the Standard Model spectrum and the extra composites below the electroweak scale. Considering the effective theory cutoff at Λ=4πv3\Lambda = 4\pi v \sim 3 TeV, consistency with the TT and SS parameters and the newly observed HγγH\to \gamma\gamma can be found for a rather restricted range of masses of vector and axial-vector composites from 1.51.5 TeV to 1.71.7 TeV and 1.81.8 TeV to 1.91.9 TeV, respectively, and only provided a non-standard kinetic mixing between the W3W^{3} and B0B^{0} fields is included.Comment: 30 pages, 10 figures. Version for publication in European Physical Journal

    A Characterization of concave mappings

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    This study focuses on Concave mappings, a class of univalent functions that exhibit a unique property: they map the unit disk onto a domain whose complement is convex. The main objective of this work is to characterize these mappings in terms of the real part of the expression 1+zf(z)/f(z)1 +zf''(z)/f'(z), considering scenarios where the omitted convex domain is either bounded or unbounded. In the case of a bounded convex domain, we investigate the pivotal role played by the Schwarzian derivative and the order of the functions in understanding the behavior and properties of these mappings

    Analysis of the quark sector in the 2HDM-III with a four-zero Yukawa texture using the most recent data on the CKM matrix

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    In this letter we analyse, in the context of the general 2-Higgs Doublet Model, the structure of the Yukawa matrices, Y~1,2q\widetilde{ \bf Y}_{ _{1,2} }^{q}, by assuming a four-zero texture ansatz for their definition. In this framework, we obtain compact expressions for Y~1,2q\widetilde{ \bf Y}_{ _{1,2} }^{q}, which are reduced to the Cheng and Sher ansatz with the difference that they are obtained naturally as a direct consequence of the invariants of the fermion mass matrices. Furthermore, in order to avoid large flavour violating effects coming from charged Higgs exchange, we consider the main flavour constraints on the off-diagonal terms of Yukawa texture {{(χ~jq)kl\left( \widetilde{\chi}_{j}^q \right)_{kl}}} (klk\neq l). We perform a χ2\chi^2-fit based on current experimental data on the quark masses and the Cabibbo-Kobayashi-Maskawa mixing matrix VCKM{ \bf V}_{\rm CKM }. Hence, we obtain the allowed ranges for the parameters Y~1,2q\widetilde{ \bf Y}_{ _{1,2} }^{q} at 1σ\sigma for several values of tanβ\tan \beta. The results are in complete agreement with the bounds obtained taking into account constraints on Flavour Changing Neutral Currents reported in the literature.Comment: 12 pages, 1 figure. Version accepted in Phys. Lett.

    Phase diagram of silicon from atomistic simulations

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    In this letter we present a calculation of the temperature-pressure phase diagram of Si in a range of pressures covering from -5 to 20 GPa and temperatures up to the melting point. The phase boundaries and triple points between the diamond, liquid, β\beta-Sn and Si34{Si}_{34} clathrate phases are reported. We have employed efficient simulation techniques to calculate free energies and to numerically integrate the Clausius-Clapeyron equation, combined with a tight binding model capable of an accuracy comparable to that of first-principles methods. The resulting phase diagram agrees well with the available experimental data.Comment: 5 pages, 1 figure, accepted in PR
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