8,450 research outputs found

    Large pseudoscalar Yukawa couplings in the complex 2HDM

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    We start by presenting the current status of a complex flavour conserving two-Higgs doublet model. We will focus on some very interesting scenarios where unexpectedly the light Higgs couplings to leptons and to b-quarks can have a large pseudoscalar component with a vanishing scalar component. Predictions for the allowed parameter space at end of the next run with a total collected luminosity of 300fb1300 \, fb^{-1} and 3000fb13000 \, fb^{-1} are also discussed. These scenarios are not excluded by present data and most probably will survive the next LHC run. However, a measurement of the mixing angle ϕτ\phi_\tau, between the scalar and pseudoscalar component of the 125 GeV Higgs, in the decay hτ+τh \to \tau^+ \tau^- will be able to probe many of these scenarios, even with low luminosity. Similarly, a measurement of ϕt\phi_t in the vertex tˉth\bar t t h could help to constrain the low tanβ\tan \beta region in the Type I model.Comment: 21 pages, 10 figure

    Construção em altura com MLCC

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    Com o objetivo de dar resposta aos problemas identificados nas soluções e propostas já conhecidas, e como parte resultante de uma investigação sobre a construção em altura com MLCC a decorrer na Escola de Engenharia da Universidade do Minho (EEUM), encontra-se em desenvolvimento o Urban Timber System (UT System)

    CP violation in 2HDM and EFT: the ZZZ vertex

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    We study the CP violating ZZZ vertex in the two-Higgs doublet model, which is a probe of a Jarlskog-type invariant in the extended Higgs sector. The form factor f4Zf_4^Z is evaluated at one loop in a general RξR_\xi gauge and its magnitude is estimated in the realistic parameter space. Then we turn to the decoupling limit of the two-Higgs doublet model, where the extra scalars are heavy and the physics can be described by the Standard Model supplemented by higher-dimensional operators. The leading operator contributing to f4Zf_4^Z at one loop is identified. The CP violating ZZZ vertex is not generated in the effective theory by dimension-8 operators, but instead arises only at the dimension-12 level, which implies an additional suppression by powers of the heavy Higgs mass scale.Comment: 21 pages; v2: added references and comments, appendix A on method of regions, and appendix B on derivation of CP-violating effective Lagrangian. Corrected discussion of dimension-12 operators contributing to ZZZ vertex. Final JHEP versio

    Blind Compressed Sensing Over a Structured Union of Subspaces

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    This paper addresses the problem of simultaneous signal recovery and dictionary learning based on compressive measurements. Multiple signals are analyzed jointly, with multiple sensing matrices, under the assumption that the unknown signals come from a union of a small number of disjoint subspaces. This problem is important, for instance, in image inpainting applications, in which the multiple signals are constituted by (incomplete) image patches taken from the overall image. This work extends standard dictionary learning and block-sparse dictionary optimization, by considering compressive measurements, e.g., incomplete data). Previous work on blind compressed sensing is also generalized by using multiple sensing matrices and relaxing some of the restrictions on the learned dictionary. Drawing on results developed in the context of matrix completion, it is proven that both the dictionary and signals can be recovered with high probability from compressed measurements. The solution is unique up to block permutations and invertible linear transformations of the dictionary atoms. The recovery is contingent on the number of measurements per signal and the number of signals being sufficiently large; bounds are derived for these quantities. In addition, this paper presents a computationally practical algorithm that performs dictionary learning and signal recovery, and establishes conditions for its convergence to a local optimum. Experimental results for image inpainting demonstrate the capabilities of the method
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