6,482 research outputs found

    Uniform W^{1,p} Estimates for Systems of Linear Elasticity in a Periodic Medium

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    Let LΟ΅\mathcal{L}_\epsilon be a family of elliptic systems of linear elasticity with rapidly oscillating periodic coefficients. We obtain the uniform W1,pW^{1,p} estimate in a Lipschitz domain for solutions to the Dirichlet problem, where (2n/(n+1))βˆ’Ξ΄<p<(2n/(nβˆ’1))+Ξ΄(2n/(n+1)) -\delta<p<(2n/(n-1))+\delta. The ranges of pp's are sharp for n=2n=2 or 3

    Non-leptonic two-body weak decays of Ξ›c(2286)\Lambda_c(2286)

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    We study the non-leptonic two-body weak decays of Ξ›c+(2286)β†’BnM\Lambda_c^+(2286)\to {\bf B}_n M with Bn{\bf B}_n (MM) representing as the baryon (meson) states. Based on the SU(3)SU(3) flavor symmetry, we can describe most of the data reexamined by the BESIII Collaboration with higher precisions. However, our result of B(Ξ›c+β†’pΟ€0)=(5.6Β±1.5)Γ—10βˆ’4{\cal B}(\Lambda_c^+ \to p\pi^0)=(5.6\pm 1.5)\times 10^{-4} is larger than the current experimental limit of 3Γ—10βˆ’43\times10^{-4} (90\% C.L.) by BESIII. In addition, we find that B(Ξ›c+β†’Ξ£+K0)=(8.0Β±1.6)Γ—10βˆ’4{\cal B}(\Lambda_c^+ \to \Sigma^+ K^0)=(8.0\pm 1.6)\times 10^{-4}, B(Ξ›c+β†’Ξ£+Ξ·β€²)=(1.0βˆ’0.8+1.6)Γ—10βˆ’2{\cal B}(\Lambda_c^+ \to \Sigma^+ \eta^\prime)=(1.0^{+1.6}_{-0.8})\times 10^{-2}, and B(Ξ›c+β†’pΞ·β€²)=(12.2βˆ’β€‰β€‰β€‰8.7+14.3)Γ—10βˆ’4{\cal B}(\Lambda_c^+ \to p \eta^\prime)=(12.2^{+14.3}_{-\,\,\,8.7})\times 10^{-4}, which are accessible to the BESIII experiments.Comment: 12 pages, 1 figure, revised version accepted by PL

    Matter Power Spectra in Viable f(R)f(R) Gravity Models with Massive Neutrinos

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    We investigate the matter power spectra in the power law and exponential types of viable f(R)f(R) theories along with massive neutrinos. The enhancement of the matter power spectrum is found to be a generic feature in these models. In particular, we show that in the former type, such as the Starobinsky model, the spectrum is magnified much larger than the latter one, such as the exponential model. A greater scale of the total neutrino mass, Ξ£mΞ½\Sigma m_{\nu}, is allowed in the viable f(R)f(R) models than that in the Ξ›\LambdaCDM one. We obtain the constraints on the neutrino masses by using the CosmoMC package with the modified MGCAMB. Explicitly, we get $\Sigma m_{\nu} < 0.451 \ (0.214)\ \mathrm{eV}at95thecorrespondingoneforthe at 95% C.L. in the Starobinsky (exponential) model, while the corresponding one for the \LambdaCDMmodelisCDM model is \Sigma m_{\nu} < 0.200\ \mathrm{eV}.Furthermore,bytreatingtheeffectivenumberofneutrinospecies. Furthermore, by treating the effective number of neutrino species N_{\mathrm{eff}}asafreeparameteralongwith as a free parameter along with \Sigma m_{\nu},wefindthat, we find that N_{\mathrm{eff}} = 3.78^{+0.64}_{-0.84} (3.47^{+0.74}_{-0.60})and and \Sigma m_{\nu} = 0.533^{+0.254}_{-0.411}( (< 0.386) \ \mathrm{eV}$ at 95% C.L. in the Starobinsky (exponential) model.Comment: 15 pages, 5 figures, updated version accepted by PL

    Developing Web Services Using Workflow Model: An Inter-organizational Perspective

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    This paper discusses how a workflow model can be used in the design and development of web services composition. We particularly investigate the development of web services composition in an inter-organizational workflow environment. We discuss respectively how to design an inter-organizational workflow from scratch when there is no existing internal workflow, and how to make existing internal workflows work together in an inter-organizational workflow environment
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