9,044 research outputs found

    Peak shifts due to B(βˆ—)βˆ’BΛ‰(βˆ—)B^{(*)}-\bar{B}^{(*)} rescattering in Ξ₯(5S)\Upsilon(5S) dipion transitions

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    We study the energy distributions of dipion transitions Ξ₯(5S)\Upsilon(5S) to Ξ₯(1S,2S,3S)Ο€+Ο€βˆ’\Upsilon(1S,2S,3S)\pi^+\pi^- in the final state rescattering model. Since the Ξ₯(5S)\Upsilon(5S) is well above the open bottom thresholds, the dipion transitions are expected to mainly proceed through the real processes Ξ₯(5S)β†’B(βˆ—)BΛ‰(βˆ—)\Upsilon(5S)\to B^{(*)}\bar{B}^{(*)} and B(βˆ—)BΛ‰(βˆ—)β†’Ξ₯(1S,2S,3S)Ο€+Ο€βˆ’B^{(*)}\bar{B}^{(*)}\to \Upsilon(1S,2S,3S)\pi^+\pi^-. We find that the energy distributions of Ξ₯(1S,2S,3S)Ο€+Ο€βˆ’\Upsilon(1S,2S,3S)\pi^+\pi^- markedly differ from that of Ξ₯(5S)β†’B(βˆ—)BΛ‰(βˆ—)\Upsilon(5S)\to B^{(*)}\bar{B}^{(*)}. In particular, the resonance peak will be pushed up by about 7-20 MeV for these dipion transitions relative to the main hadronic decay modes. These predictions can be used to test the final state rescattering mechanism in hadronic transitions for heavy quarkonia above the open flavor thresholds.Comment: Version published in PRD, energy dependence of the total width in Eq.(12) restored and corresponding figure changed, more discussion and clarification adde

    Multi-view Regularized Gaussian Processes

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    Gaussian processes (GPs) have been proven to be powerful tools in various areas of machine learning. However, there are very few applications of GPs in the scenario of multi-view learning. In this paper, we present a new GP model for multi-view learning. Unlike existing methods, it combines multiple views by regularizing marginal likelihood with the consistency among the posterior distributions of latent functions from different views. Moreover, we give a general point selection scheme for multi-view learning and improve the proposed model by this criterion. Experimental results on multiple real world data sets have verified the effectiveness of the proposed model and witnessed the performance improvement through employing this novel point selection scheme

    Distributed Learning over Unreliable Networks

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    Most of today's distributed machine learning systems assume {\em reliable networks}: whenever two machines exchange information (e.g., gradients or models), the network should guarantee the delivery of the message. At the same time, recent work exhibits the impressive tolerance of machine learning algorithms to errors or noise arising from relaxed communication or synchronization. In this paper, we connect these two trends, and consider the following question: {\em Can we design machine learning systems that are tolerant to network unreliability during training?} With this motivation, we focus on a theoretical problem of independent interest---given a standard distributed parameter server architecture, if every communication between the worker and the server has a non-zero probability pp of being dropped, does there exist an algorithm that still converges, and at what speed? The technical contribution of this paper is a novel theoretical analysis proving that distributed learning over unreliable network can achieve comparable convergence rate to centralized or distributed learning over reliable networks. Further, we prove that the influence of the packet drop rate diminishes with the growth of the number of \textcolor{black}{parameter servers}. We map this theoretical result onto a real-world scenario, training deep neural networks over an unreliable network layer, and conduct network simulation to validate the system improvement by allowing the networks to be unreliable

    Zc(3900)Z_c(3900) as a DDΛ‰βˆ—D\bar{D}^* molecule from the pole counting rule

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    A comprehensive study on the nature of the Zc(3900)Z_c(3900) resonant structure is carried out in this work. By constructing the pertinent effective Lagrangians and considering the important final-state-interaction effects, we first give a unified description to all the relevant experimental data available, including the J/ΟˆΟ€J/\psi\pi and ππ\pi\pi invariant mass distributions from the e+eβˆ’β†’J/ΟˆΟ€Ο€e^+e^-\to J/\psi\pi\pi process, the hcΟ€h_c\pi distribution from e+eβˆ’β†’hcππe^+e^-\to h_c\pi\pi and also the DDΛ‰βˆ—D\bar D^{*} spectrum in the e+eβˆ’β†’DDΛ‰βˆ—Ο€e^+e^-\to D\bar D^{*}\pi process. After fitting the unknown parameters to the previous data, we search the pole in the complex energy plane and find only one pole in the nearby energy region in different Riemann sheets. Therefore we conclude that Zc(3900)Z_c(3900) is of DDΛ‰βˆ—D\bar D^* molecular nature, according to the pole counting rule method~[Nucl.~Phys.~A543, 632 (1992); Phys.~Rev.~D 35,~1633 (1987)]. We emphasize that the conclusion based upon the pole counting method is not trivial, since both the DDΛ‰βˆ—D\bar D^{*} contact interactions and the explicit ZcZ_c exchanges are introduced in our analyses and they lead to the same conclusion.Comment: 21 pages, 9 figures. To match the published version in PRD. Additional discussion on the spectral density function is include
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