6,003 research outputs found

    A Hybrid Neural Network Framework and Application to Radar Automatic Target Recognition

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    Deep neural networks (DNNs) have found applications in diverse signal processing (SP) problems. Most efforts either directly adopt the DNN as a black-box approach to perform certain SP tasks without taking into account of any known properties of the signal models, or insert a pre-defined SP operator into a DNN as an add-on data processing stage. This paper presents a novel hybrid-NN framework in which one or more SP layers are inserted into the DNN architecture in a coherent manner to enhance the network capability and efficiency in feature extraction. These SP layers are properly designed to make good use of the available models and properties of the data. The network training algorithm of hybrid-NN is designed to actively involve the SP layers in the learning goal, by simultaneously optimizing both the weights of the DNN and the unknown tuning parameters of the SP operators. The proposed hybrid-NN is tested on a radar automatic target recognition (ATR) problem. It achieves high validation accuracy of 96\% with 5,000 training images in radar ATR. Compared with ordinary DNN, hybrid-NN can markedly reduce the required amount of training data and improve the learning performance

    Branching Fractions and CP Asymmetries of the Quasi-Two-Body Decays in Bsβ†’K0(Kβ€Ύ0)KΒ±Ο€βˆ“B_{s} \to K^0(\overline K^0)K^\pm \pi^\mp within PQCD Approach

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    Motivated by the first untagged decay-time-integrated amplitude analysis of Bsβ†’KSKβˆ“Ο€Β±B_s \to K_SK^{\mp}\pi^{\pm} decays performed by LHCb collaboration, where the decay amplitudes are modeled to contain the resonant contributions from intermediate resonances Kβˆ—(892)K^*(892), K0βˆ—(1430)K_0^*(1430) and K2βˆ—(1430)K_2^*(1430), we comprehensively investigate the quasi-two-body Bsβ†’K0/Kβ€Ύ0KΒ±Ο€βˆ“B_{s} \to K^0/\overline{\kern -0.2em K}^0 K^{\pm}\pi^{\mp} decays, and calculate the branching fractions and the time-dependent CPCP asymmetries within the perturbative QCD approach based on the kTk_T factorization. In the quasi-two-body space region the calculated branching fractions with the considered intermediate resonances are in good agreement with the experimental results of LHCb by adopting proper KΟ€K\pi pair wave function, describing the interaction between the kaon and pion in the KΟ€K\pi pair. Furthermore,within the obtained branching fractions of the quasi-two-body decays, we also calculate the branching fractions of corresponding two-body decays, and the results consist with the LHCb measurements and the earlier studies with errors. For these considered decays, since the final states are not flavour-specific, the time-dependent CPCP could be measured. We calculate six CPCP-violation observables, which can be tested in the ongoing LHCb experiment.Comment: 20 page

    Cabibbo-Kobayashi-Maskawa-favored BB decays to a scalar meson and a DD meson

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    Within the perturbative QCD approach, we investigated the Cabibbo-Kobayashi-Maskawa-favored Bβ†’Dβ€ΎSB \to \overline{D} S ("SS" denoting the scalar meson) decays on the basis of the two-quark picture. Supposing the scalar mesons are the ground states or the first excited states, we calculated the the branching ratios of 72 decay modes. Most of the branching ratios are in the range 10βˆ’410^{-4} to 10βˆ’710^{-7}, which can be tested in the ongoing LHCb experiment and the forthcoming Belle-II experiment. Some decays, such as B+β†’Dβ€Ύ(βˆ—)0a0+(980/1450)B^+ \to \overline{D}^{(*)0} a_0^+(980/1450) and B+β†’D(βˆ—)βˆ’a0+(980/1450)B^+ \to D^{(*)-} a_0^+(980/1450), could be used to probe the inner structure and the character of the scalar mesons, if the experiments are available. In addition, the ratios between the Br(B0β†’Dβ€Ύ(βˆ—)0Οƒ)Br(B^0\to \overline{D}^{(*)0}\sigma) and Br(B0β†’Dβ€Ύ(βˆ—)0f0(980))Br(B^0\to \overline{D}^{(*)0}f_0(980)) provide a potential way to determine the mixing angle between Οƒ\sigma and f0(980)f_0(980). Moreover, since in the standard model these decays occur only through tree operators and have no CPCP asymmetries, any deviation will be signal of the new physics beyond the standard model.Comment: 2 figures, 6 table
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