1,729 research outputs found

    Cosmology of Antisymmetric Tensor Field in D-brane Universe

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    We analyze homogeneous, anisotropic cosmology driven by a self-interacting ``massive'' antisymmetric tensor field BμνB_{\mu\nu} which is present in string theories with D-branes. Time-dependent magnetic BB field existing in the early universe can lead to the Bianchi type I universe. Evolutions of such a tensor field are solved exactly or numerically in the universe dominated by vacuum energy, radiation, and BB field itself. The matter-like behavior of the BB field (dubbed as ``BB-matter'') ensures that the anisotropy disappears at late time and thus becomes unobservable in a reasonable cosmological scenario. Such a feature should be contrasted to the cosmology of the conventional massless antisymmetric tensor field.Comment: 13 page

    Searching for Flavored Gauge Bosons

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    Standard Model may allow an extended gauge sector with anomaly-free flavored gauge symmetries, such as Li−LjL_{i} - L_{j}, Bi−LjB_{i} - L_{j}, and B−3LiB - 3L_{i}, where i,j=1,2,3i,j=1,2,3 are flavor indices. We investigate phenomenological implications of the new flavored gauge boson Z′Z^{\prime} in the above three classes of gauge symmetries. Focusing on the gauge boson mass above 5 GeV, we use the lepton universality test in the ZZ and τ/μ\tau/\mu decays, LEP searches, LHC searches, neutrino trident production bound, and LHC Z→4μZ\rightarrow 4\mu searches to put constraints on the g′−MZ′g^{\prime}-M_{Z^{\prime}} plane. When L1L_1 is involved, the LEP bounds on the e−e+→ℓ−ℓ+e^{-}e^{+} \rightarrow \ell^{-}\ell^{+} processes give the most stringent bounds, while the LHC bound becomes the strongest constraints in the large MZ′M_{Z^{\prime}} region when BiB_{i} is involved. The bound from Z→4μZ\rightarrow 4\mu productions, which is applicable for L2L_2-involved scenarios, provides stringent bounds in the small MZ′M_{Z^{\prime}} region. One exception is the B−3L2B-3L_2 scenario, in which case only a small region is favored due to the lepton universality.Comment: v3: updated LHC bounds for B-3L_i model

    String Cosmology of the D-brane Universe

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    We analyze homogeneous anisotropic cosmology driven by the dilaton and the self-interacting ``massive'' antisymmetric tensor field which are indispensable bosonic degrees with the graviton in the NS-NS sector of string theories with D-branes. We found the attractor solutions for this system, which show the overall features of general solutions, and confirmed it through numerical analysis. The dilaton possesses the potential due to the presence of the D-brane and the curvature of extra dimensions. In the presence of the non-vanishing antisymmetric tensor field, the homogeneous universe expands anisotropically while the D-brane term dominates. The isotropy is recovered as the dilaton rolls down and the curvature term dominates. With the stabilizing potential for the dilaton, the isotropy can also be recovered.Comment: 23 pages, 8 figures. Final version, to appear in Phys. Rev.

    Cosmology of Light Moduli

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    In string/M-theory with a large compactification radius, some axion-like moduli can be much lighter than the gravitino. Generic moduli in gauge-mediated supersymmetry breaking models also have a mass far below the weak scale. Motivated by these, we examine the cosmological implications of light moduli for the mass range from the weak scale to an extremely small scale of order 10^{-26} eV, and obtain an upper bound on the initial moduli misalignment for both cases with and without a late entropy production.Comment: 23 pages including 3 pictex-figures, Late

    Axino-Neutrino Mixing in Gauge-Mediated Supersymmetry Breaking Models

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    When the strong CP problem is solved by spontaneous breaking of an anomalous global symmetry in theories with gauge-mediated supersymmetry breaking, the pseudo Goldstone fermion (the axino) is a good candidate of a light sterile neutrino. Its mixing with neutrinos relevant for current neutrino experiments can arise in the presence of R-parity violation. The realistic four neutrino mass matrix is obtained when the see-saw mechanism is brought in, and an ansatz for the right-handed neutrino mass is constructed.Comment: Revtex, 7 pp. Version to appear in Phys. Lett.
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