7,234 research outputs found

    Hosotani mechanism on the lattice

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    We explore the phase structure and symmetry breaking in four-dimensional SU(3) gauge theory with one spatial compact dimension on the lattice in the presence of fermions in the adjoint and fundamental representations with general boundary conditions. The eigenvalue phases of Polyakov loops and the associated susceptibility are measured on 16^3 x 4 lattice. We establish a correspondence between the phases found on the lattice and the gauge symmetry breaking by the Hosotani mechanism.Comment: 7 pages, 4 figures, prepared for the 31st International Symposium on Lattice Field Theory - LATTICE 2013 Added preprint number

    Nonuniversal ZZ^{\prime} couplings in B decays

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    We study the impacts of nonuniversal ZZ^{\prime} model, providing flavor changing neutral current at tree level, on the branching ratios (BRs), CP asymmetries (CPAs) and polarization fractions of B decays. We find that for satisfying the current data, the new left- and right-handed couplings have to be included at the same time. The new introduced effective interactions not only could effectively explain the puzzle of small longitudinal polarization in BKϕB\to K^* \phi decays, but also provide a solution to the small CPA of B±π0K±B^{\pm}\to \pi^{0} K^{\pm}. We also find that the favorable CPA of B±π0K±B^{\pm}\to \pi^{0} K^{\pm} is opposite in sign to the standard model; meanwhile, the CPA of Bdπ0KB_{d}\to \pi^{0}K has to be smaller than -10%. In addition, by using the values of parameters which are constrained by BπKB\to \pi K, we find that the favorable ranges of BRs, CPAs, longitudinal polarizations, and perpendicular transverse polarizations for (B±ρ±K,BdρK±)(B^{\pm}\to \rho^{\pm} K^{*}, B_{d}\to \rho^{\mp} K^{*\pm}) are (17.1±3.9,10.0±2.0)×106(17.1\pm 3.9, 10.0\pm2.0)\times 10^{-6}, (3±5,21±7)(3\pm 5, 21\pm 7)%, (0.66±0.10,0.44±0.08)(0.66\pm 0.10, 0.44\pm 0.08) and (0.14±0.10,0.25±0.09)(0.14\pm 0.10, 0.25\pm 0.09), respectively.Comment: 28 pages, 9 figures, version revise
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