50,169 research outputs found

    Effect of nickel on the microstructure and mechanical property of die-cast Al–Mg–Si–Mn alloy

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    The effect of nickel on the microstructure and mechanical properties of a die-cast Al–Mg–Si–Mn alloy has been investigated. The results show that the presence of Ni in the alloy promotes the formation of Ni-rich intermetallics. These occur consistently during solidification in the die-cast Al–Mg–Si–Mn alloy across different levels of Ni content. The Ni-rich intermetallics exhibit dendritic morphology during the primary solidification and lamellar morphology during the eutectic solidification stage. Ni was found to be always associated with iron forming AlFeMnSiNi intermetallics, and no Al3Ni intermetallic was observed when Ni concentrations were up to 2.06 wt% in the alloy. Although with different morphologies, the Ni-rich intermetallics were identified as the same AlFeMnSiNi phase bearing a typical composition of Al[100–140](Fe,Mn)[2–7]SiNi[4–9]. With increasing Ni content, the spacing of the α-Al–Mg2Si eutectic phase was enlarged in the Al–Mg–Si–Mn alloy. The addition of Ni to the alloy resulted in a slight increase in the yield strength, but a significant decrease in the elongation. The ultimate tensile strength (UTS) increased slightly from 300 to 320 MPa when a small amount (e.g. 0.16 wt%) of Ni was added to the alloy, but further increase of the Ni content resulted in a decrease of the UTS.The Engineering and Physical Sciences Research Council (EPSRC), Technology Strategy Board (TSB) and Jaguar Land Rover (JLR) in the United Kingdom

    Lorentz Symmetry and the Internal Structure of the Nucleon

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    To investigate the internal structure of the nucleon, it is useful to introduce quantities that do not transform properly under Lorentz symmetry, such as the four-momentum of the quarks in the nucleon, the amount of the nucleon spin contributed by quark spin, etc. In this paper, we discuss to what extent these quantities do provide Lorentz-invariant descriptions of the nucleon structure.Comment: 6 pages, no figur

    Neural network determination of the non-singlet quark distribution

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    We summarize the main features of our approach to parton fitting, and we show a preliminary result for the non-singlet structure function. When comparing our result to other PDF sets, we find a better description of large x data and larger error bands in the extrapolation regions.Comment: 4 pages, 1 eps figure. Presented at the XIV International Workshop on Deep Inelastic Scattering (DIS2006), Tsukuba, Japan, 20-24 April 200

    Distribution amplitudes and decay constants for (π,K,ρ,K)(\pi,K,\rho,K^*) mesons in light-front quark model

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    We present a calculation of the quark distribution amplitudes(DAs), the Gegenbauer moments, and decay constants for π,ρ,K\pi,\rho,K and KK^* mesons using the light-front quark model. While the quark DA for π\pi is somewhat broader than the asymptotic one, that for ρ\rho meson is very close to the asymptotic one. The quark DAs for KK and KK^* show asymmetric form due to the flavor SU(3)-symmetry breaking effect. The decay constants for the transversely polarized ρ\rho and KK^* mesons(fρTf^T_\rho and fKTf^T_{K^*}) as well as the longitudinally polarized ones(fρf_\rho and fKf_{K^*}) are also obtained. Our averaged values for fVT/fVf^T_V/f_V, i.e. (fρT/fρ)av=0.78(f^T_\rho/f_\rho)_{\rm av}=0.78 and (fKT/fK)av=0.84(f^T_{K^*}/f_{K^*})_{\rm av}=0.84, are found to be consistent with other model predictions. Especially, our results for the decay constants are in a good agreement with the SU(6) symmetry relation, fρ(K)T=(fπ(K)+fρ(K))/2f^T_{\rho(K^*)}=(f_{\pi(K)}+f_{\rho(K^*)})/2.Comment: 12 pages, 6figure
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