13,060 research outputs found

    Delayed Onset and Fast Rise of Prompt Optical-UV Emission from Gamma-Ray Bursts in Molecular Clouds

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    Observations imply that long \gamma-ray bursts (GRBs) are originated from explosions of massive stars, therefore they may occur in the molecular clouds where their progenitors were born. We show here that the prompt optical-UV emission from GRBs may be delayed due to the dust extinction, which can well explain the observed optical delayed onset and fast rise in GRB 080319B. The density and the size of the molecular cloud around GRB 080319B are roughly constrained to be \sim10^3cm^{-3} and \sim 8pc, respectively. We also investigate the other GRBs with prompt optical-UV data, and find similar values of the densities and sizes of the local molecular clouds. The future observations of prompt optical-UV emission from GRBs in subsecond timescale, e.g., by UFFO-Pathfinder and SVOM-GWAC, will provide more evidence and probes of the local GRB environments.Comment: 15 pages, 5 figures, RAA 13 (2013) 57-70, typo correctio

    Implications on Ξ·\eta-Ξ·β€²\eta'-glueball mixing from Bd/sβ†’J/Ψη(β€²)B_{d/s} \to J/\Psi \eta^{(')} Decays

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    We point out that the recent Belle measurements of the Bd/sβ†’J/Ψη(β€²)B_{d/s} \to J/\Psi \eta^{(')} decays imply large pseudoscalar glueball contents in the Ξ·(β€²)\eta^{(\prime)} meson. These decays are studied in the perturbative QCD (PQCD) approach, considering the Ξ·\eta-Ξ·β€²\eta'-GG mixing, where GG represents the pseudoscalar glueball. It is shown that the PQCD predictions for the Bd/sβ†’J/Ψη(β€²)B_{d/s} \to J/\Psi \eta^{(')} branching ratios agree well with the data for the mixing angle Ο•Gβ‰ˆ30∘\phi_G\approx 30^\circ between the flavor-singlet state and the pure pseudoscalar glueball. Extending the formalism to the Ξ·\eta-Ξ·β€²\eta'-GG-Ξ·c\eta_c tetramixing, the abnormally large observed Bdβ†’KΞ·β€²B_d\to K\eta' branching ratios are also explained. The proposed mixing formalism is applicable to other heavy meson decays into Ξ·(β€²)\eta^{(\prime)} mesons, and could be tested by future LHCb and Super-BB factory data.Comment: Improved version, references added, 7 pages, 1 figur

    Study of the weak annihilation contributions in charmless Bs→VVB_s\to VV decays

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    In this paper, in order to probe the spectator-scattering and weak annihilation contributions in charmless Bsβ†’VVB_s\to VV (where VV stands for a light vector meson) decays, we perform the Ο‡2\chi^2-analyses for the end-point parameters within the QCD factorization framework, under the constraints from the measured BΛ‰sβ†’\bar B_{s}\toρ0Ο•\rho^0\phi, Ο•Kβˆ—0\phi K^{*0}, ϕϕ\phi \phi and Kβˆ—0KΛ‰βˆ—0K^{*0}\bar K^{*0} decays. The fitted results indicate that the end-point parameters in the factorizable and nonfactorizable annihilation topologies are non-universal, which is also favored by the charmless Bβ†’PPB\to PP and PVPV (where PP stands for a light pseudo-scalar meson) decays observed in the previous work. Moreover, the abnormal polarization fractions fL,βŠ₯(BΛ‰sβ†’Kβˆ—0KΛ‰βˆ—0)=(20.1Β±7.0)% ,(58.4Β±8.5)%f_{L,\bot}(\bar B_{s}\to K^{*0}\bar K^{*0})=(20.1\pm7.0)\%\,,(58.4\pm8.5)\% measured by the LHCb collaboration can be reconciled through the weak annihilation corrections. However, the branching ratio of BΛ‰sβ†’Ο•Kβˆ—0\bar B_{s}\to\phi K^{*0} decay exhibits a tension between the data and theoretical result, which dominates the contributions to Ο‡min2\chi_{\rm min}^2 in the fits. Using the fitted end-point parameters, we update the theoretical results for the charmless Bsβ†’VVB_s\to VV decays, which will be further tested by the LHCb and Belle-II experiments in the near future.Comment: 31 pages, 4 figures, 6 table
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