183 research outputs found

    Decentralized Approximate Bayesian Inference for Distributed Sensor Network

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    Bayesian models provide a framework for probabilistic modelling of complex datasets. Many such models are computationally demanding, especially in the presence of large datasets. In sensor network applications, statistical (Bayesian) parameter estimation usually relies on decentralized algorithms, in which both data and computation are distributed across the nodes of the network. In this paper we propose a framework for decentralized Bayesian learning using Bregman Alternating Direction Method of Multipliers (B-ADMM).We demonstrate the utility of our framework, with Mean Field Variational Bayes (MFVB) as the primitive for distributed affine structure from motion (SfM).Peer reviewe

    Facial Augmentation with Implants

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    Contemporary Rhinoplasty Techniques

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    Revision Rhinoplasty

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    Multi-operated Nose

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    Controversies in Modern Rhinoplasty

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    Estimating the branching fraction for B0ψ(2S)π0B^0\rightarrow \psi(2S)\pi^0 decay

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    I present estimates of the branching fractions in the non-leptonic charmonium two-body decay rates for B0ψ(2S)π0B^0\rightarrow \psi(2S)\pi^0 decay and the same decays of B+ψ(2S)π+B^+\rightarrow \psi(2S)\pi^+, B0ψ(2S)K0B^0\rightarrow \psi(2S)K^0 and B+ψ(2S)K+B^+\rightarrow \psi(2S)K^+. These estimates are based on a generalized factorization approach making use of leading order (LO) and next-to-leading order (NLO) contributions. I find that when the large enhancements from the known NLO contributions by using the QCD factorization approach are taken into account, the branching ratios are the following: Br(B0ψ(2S)π0)=(1.067±0.059)×105Br(B^0\rightarrow \psi(2S)\pi^0)=(1.067\pm0.059)\times10^{-5}, Br(B+ψ(2S)π+)=(2.134±0.0.118)×105Br(B^+\rightarrow \psi(2S)\pi^+)=(2.134\pm0.0.118)\times10^{-5}, Br(B0ψ(2S)K0)=(6.344±0.376)×104Br(B^0\rightarrow \psi(2S)K^0)=(6.344\pm0.376)\times10^{-4} and Br(B+ψ(2S)K+)=(6.344±0.376)×104Br(B^+\rightarrow \psi(2S)K^+)=(6.344\pm0.376)\times10^{-4}, while the experimental results are (1.17±0.17)×105(1.17\pm 0.17)\times 10^{-5}, (2.44±0.30)×105(2.44\pm 0.30)\times 10^{-5}, (6.20±0.50)×104(6.20\pm 0.50)\times 10^{-4} and (6.39±0.33)×104(6.39\pm 0.33)\times 10^{-4} respectively. All estimates are in good agreement with the experimental results.Comment: Repeated topi
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