3,288 research outputs found

    Bound Energy Masses of Mesons Containing the Fourth Generation and Iso-singlet Quarks

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    The fourth Standard Model (SM) family quarks and weak iso-singlet quarks The fourth Standard Model (SM) family quarks and weak iso-singlet quarks predicted by E6{\rm E}_{6\text{}} GUT are considered. The spin-average of the pseudoscalar η4(n1S0)\eta_{4}(n^{1}S_{0}) and vector ψ4(n3S1)\psi_{4}(n^{3}S_{1}) quarkonium binding masses of the new mesons formed by the fourth Standard Model (SM) family and iso-singlet E6{\rm E}_{6\text{}} with their mixings to ordinary quarks are investigated. Further, the fine and hyperfine mass splittings of the these states are also calculated. We solved the Schr\"{o}dinger equation with logarithmic and Martin potentials using the Shifted large-N{\rm N} expansion technique. Our results are compared with other models to gauge the reliability of the predictions and point out differences.Comment: 13 page

    A Systematic Study on Nonrelativistic Quarkonium Interaction

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    recently proposed strictly phenomenological static quark-antiquark potential belonging to the generality V(r)=Arα+κrβ+V0V(r)=-Ar^{-\alpha}+\kappa r^{\beta}+V_{0} is tested with heavy quarkonia in the context of the shifted large N-expansion method. This nonrelativistic potential model fits the spin-averaged mass spectra of the ccˉ,c\bar{c}, bbˉb\bar{b} and cc% \bar{b} quarkonia within a few MeV{\rm MeV} and also the five experimentally known leptonic decay widths of the ccˉc\bar{c} and bb% \bar{b} vector states. Further, we compute the hyperfine splittings of the bottomonium spectrum as well as the fine and hyperfine splittings of the charmonium spectrum. We give predictions for not yet observed BcB_{c} splittings. The model is then used to predict the masses of the remaining quarkonia and the leptonic decay widths of the two pseudoscalar c\bar{b%} states. Our results are compared with other models to gauge the reliability of the predictions and point out differences.Comment: 24 page

    New exact solution of the one dimensional Dirac Equation for the Woods-Saxon potential within the effective mass case

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    We study the one-dimensional Dirac equation in the framework of a position dependent mass under the action of a Woods-Saxon external potential. We find that constraining appropriately the mass function it is possible to obtain a solution of the problem in terms of the hypergeometric function. The mass function for which this turns out to be possible is continuous. In particular we study the scattering problem and derive exact expressions for the reflection and transmission coefficients which are compared to those of the constant mass case. For the very same mass function the bound state problem is also solved, providing a transcendental equation for the energy eigenvalues which is solved numerically.Comment: Version to match the one which has been accepted for publication by J. Phys. A: Math. Theor. Added one figure, several comments and few references. (24 pages and 7 figures

    Path Integral Solution of PT-/non-PT-Symmetric and non-Hermitian Hulthen Potential

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    The wave functions and the energy spectrum of PT-/non-PT-Symmetric and non-Hermitian Hulthen potential are of an exponential type and are obtained via the path integral. The path integral is constructed using parametric time and point transformation
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