44,043 research outputs found

    Electrical Neutrality and Symmetry Restoring Phase Transitions at High Density in a Two-Flavor Nambu-Jona-Lasinio Model

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    A general research on chiral symmetry restoring phase transitions at zero temperature and finite chemical potentials under electrical neutrality condition has been conducted in a Nambu-Jona-Lasinio model to describe two-flavor normal quark matter. Depending on that m0/Λm_0/\Lambda, the ratio of dynamical quark mass in vacuum and the 3D momentum cutoff in the loop integrals, is less or greater than 0.413, the phase transition will be second or first order. A complete phase diagram of uu quark chemical potential versus m0m_0 is given. With the electrical neutrality constraint, the region where second order phase transition happens will be wider than the one without electrical neutrality limitation. The results also show that, for the value of m0/Λm_0/\Lambda from QCD phenomenology, the phase transition must be first order.Comment: 9 pages, 1 figur

    Semileptonic decays of BcB_c meson to S-wave charmonium states in the perturbative QCD approach

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    Inspired by the recent measurement of the ratio of BcB_c branching fractions to J/ψπ+J/\psi \pi^+ and J/ψμ+νμJ/\psi \mu^+\nu_{\mu} final states at the LHCb detector, we study the semileptonic decays of BcB_c meson to the S-wave ground and radially excited 2S and 3S charmonium states with the perturbative QCD approach. After evaluating the form factors for the transitions Bc→P,VB_c\rightarrow P,V, where PP and VV denote pseudoscalar and vector S-wave charmonia, respectively, we calculate the branching ratios for all these semileptonic decays. The theoretical uncertainty of hadronic input parameters are reduced by utilizing the light-cone wave function for BcB_c meson. It is found that the predicted branching ratios range from 10−610^{-6} up to 10−210^{-2} and could be measured by the future LHCb experiment. Our prediction for the ratio of branching fractions BR(Bc+→J/Ψπ+)BR(Bc+→J/Ψμ+νμ)\frac{\mathcal {BR}(B_c^+\rightarrow J/\Psi \pi^+)}{\mathcal {BR}(B_c^+\rightarrow J/\Psi \mu^+\nu_{\mu})} is in good agreement with the data. For Bc→VlνlB_c\rightarrow V l \nu_l decays, the relative contributions of the longitudinal and transverse polarization are discussed in different momentum transfer squared regions. These predictions will be tested on the ongoing and forthcoming experiments.Comment: 12 pages, 3 figures, 5 table
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