135,705 research outputs found

    The role of qqˉq\bar q components in the N(1440) resonance

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    The role of 5-quark components in the pion and electromagnetic decays and transition form factors of the N(1440) is explored. The qqqqqˉqqqq\bar q components, where the 4-quark subsystem has the flavor-spin symmetries [4]FS[22]F[22]S[4]_{FS}[22]_F[22]_S and [4]FS[31]F[31]S[4]_{FS}[31]_F[31]_S, which are expected to have the lowest energy of all qqqqqˉqqqq\bar q configurations, are considered in detail with a nonrelativistic quark model. The matrix elements between the 5-quark components of the N(1440) and the nucleon, qqqqqˉ→qqqqqˉqqqq\bar q\to qqqq\bar q, play a minor role in these decays, while the transition matrix elements qqqqqˉ→qqqqqqq\bar q\to qqq and qqq→qqqqqˉqqq\to qqqq\bar q that involve quark antiquark annihilation are very significant. Both for the electromagnetic and strong decay the change from the valence quark model value is dominated by the confinement triggered qqˉq\bar q annihilation transitions. In the case of pion decay the calculated decay width is enhanced substantially both by the direct qqˉ→πq\bar q \to \pi and also by the confinement triggered qqˉ→πq\bar q\to \pi transitions. Agreement with the empirical value for the pion decay width may be reached with a ∼\sim 30% qqqqqˉqqqq\bar q component in the N(1440).Comment: 23 pages revte

    Lattice Boltzmann modeling of multiphase flows at large density ratio with an improved pseudopotential model

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    Owing to its conceptual simplicity and computational efficiency, the pseudopotential multiphase lattice Boltzmann (LB) model has attracted significant attention since its emergence. In this work, we aim to extend the pseudopotential LB model to simulate multiphase flows at large density ratio and relatively high Reynolds number. First, based on our recent work [Li et al., Phys. Rev. E. 86, 016709 (2012)], an improved forcing scheme is proposed for the multiple-relaxation-time pseudopotential LB model in order to achieve thermodynamic consistency and large density ratio in the model. Next, through investigating the effects of the parameter a in the Carnahan-Starling equation of state, we find that the interface thickness is approximately proportional to 1/sqrt(a). Using a smaller a will lead to a wider interface thickness, which can reduce the spurious currents and enhance the numerical stability of the pseudopotential model at large density ratio. Furthermore, it is found that a lower liquid viscosity can be gained in the pseudopotential model by increasing the kinematic viscosity ratio between the vapor and liquid phases. The improved pseudopotential LB model is numerically validated via the simulations of stationary droplet and droplet oscillation. Using the improved model as well as the above treatments, numerical simulations of droplet splashing on a thin liquid film are conducted at a density ratio in excess of 500 with Reynolds numbers ranging from 40 to 1000. The dynamics of droplet splashing is correctly reproduced and the predicted spread radius is found to obey the power law reported in the literature.Comment: 9 figures, 2 tables, accepted by Physical Review E (in press

    Five-quark components in Δ(1232)→Nπ\Delta(1232)\to N\pi decay

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    Five-quark qqqqqˉqqqq\bar q components in the Δ(1232)\Delta(1232) are shown to contribute significantly to Δ(1232)→Nπ\Delta(1232)\to N\pi decay through quark-antiquark annihilation transitions. These involve the overlap between the qqqqqq and qqqqqˉqqqq\bar q components and may be triggered by the confining interaction between the quarks. With a ∼\sim 10% admixture of five-quark components in the Δ(1232)\Delta(1232) the decay width can be larger by factors 2 - 3 over that calculated in the quark model with 3 valence quarks, depending on the details of the confining interaction. The effect of transitions between the qqqqqˉqqqq\bar q components themselves on the calculated decay width is however small. The large contribution of the quark-antiquark annihilation transitions thus may compensate the underprediction of the width of the Δ(1232)\Delta(1232) by the valence quark model, once the Δ(1232)\Delta(1232) contains qqqqqˉqqqq\bar q components with ∼\sim 10% probability.Comment: accepted versio
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