4,300 research outputs found

    Analysis of the scalar, axialvector, vector, tensor doubly charmed tetraquark states with QCD sum rules

    Full text link
    In this article, we construct the axialvector-diquark-axialvector-antidiquark type currents to interpolate the scalar, axialvector, vector, tensor doubly charmed tetraquark states, and study them with QCD sum rules systematically by carrying out the operator product expansion up to the vacuum condensates of dimension 10 in a consistent way, the predicted masses can be confronted to the experimental data in the future. We can search for those doubly charmed tetraquark states in the Okubo-Zweig-Iizuka super-allowed strong decays to the charmed meson pairs.Comment: 23 pages, 29 figures. arXiv admin note: substantial text overlap with arXiv:1708.0454

    Revisit assignments of the new excited Ωc\Omega_c states with QCD sum rules

    Full text link
    In this article, we distinguish the contributions of the positive parity and negative parity Ωc\Omega_c states, study the masses and pole residues of the 1S, 1P, 2S and 2P Ωc\Omega_c states with the spin J=12J=\frac{1}{2} and 32\frac{3}{2} using the QCD sum rules in a consistent way, and revisit the assignments of the new narrow excited Ωc0\Omega_c^0 states. The predictions support assigning the Ωc(3000)\Omega_c(3000) to be the 1P Ωc\Omega_c state with JP=12J^P={\frac{1}{2}}^-, assigning the Ωc(3090)\Omega_c(3090) to be the 1P Ωc\Omega_c state with JP=32J^P={\frac{3}{2}}^- or the 2S Ωc\Omega_c state with JP=12+J^P={\frac{1}{2}}^+, and assigning Ωc(3119)\Omega_c(3119) to be the 2S Ωc\Omega_c state with JP=32+J^P={\frac{3}{2}}^+.Comment: 19 pages, 22 figures. arXiv admin note: text overlap with arXiv:1705.0774

    Magnetothermoelectric DC conductivities from holography models with hyperscaling factor in Lifshitz spacetime

    Full text link
    We investigate an Einstein-Maxwell-Dilaton-Axion holographic model and obtain two branches of a charged black hole solution with a dynamic exponent and a hyperscaling violation factor when a magnetic field presents. The magnetothermoelectric DC conductivities are then calculated in terms of horizon data by means of holographic principle. We find that linear temperature dependence resistivity and quadratic temperature dependence inverse Hall angle can be achieved in our model. The well-known anomalous temperature scaling of the Nernst signal and the Seebeck coefficient of cuprate strange metals are also discussed.Comment: 1+23 pages, 4 figures, references adde
    corecore