12,333 research outputs found

    Study of Ξ›bβ†’Ξ›(Ο•,Ξ·(β€²))\Lambda_b\to \Lambda (\phi,\eta^{(\prime)}) and Ξ›bβ†’Ξ›K+Kβˆ’\Lambda_b\to \Lambda K^+K^- decays

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    We study the charmless two-body Ξ›bβ†’Ξ›(Ο•,Ξ·(β€²))\Lambda_b\to \Lambda (\phi,\eta^{(\prime)}) and three-body Ξ›bβ†’Ξ›K+Kβˆ’\Lambda_b\to \Lambda K^+K^- decays. We obtain B(Ξ›b→Λϕ)=(3.53Β±0.24)Γ—10βˆ’6{\cal B}(\Lambda_b\to \Lambda\phi)=(3.53\pm 0.24)\times 10^{-6} to agree with the recent LHCb measurement. However, we find that B(Ξ›bβ†’Ξ›(Ο•β†’)K+Kβˆ’)=(1.71Β±0.12)Γ—10βˆ’6{\cal B}(\Lambda_b\to \Lambda(\phi\to)K^+ K^-)=(1.71\pm 0.12)\times 10^{-6} is unable to explain the LHCb observation of B(Ξ›bβ†’Ξ›K+Kβˆ’)=(15.9Β±1.2Β±1.2Β±2.0)Γ—10βˆ’6{\cal B}(\Lambda_b\to\Lambda K^+ K^-)=(15.9\pm 1.2\pm 1.2\pm 2.0)\times 10^{-6}, which implies the possibility for other contributions, such as that from the resonant Ξ›bβ†’Kβˆ’Nβˆ—, Nβˆ—β†’Ξ›K+\Lambda_b\to K^- N^*,\,N^*\to\Lambda K^+ decay with Nβˆ—N^* as a higher-wave baryon state. For Ξ›b→Λη(β€²)\Lambda_b\to \Lambda \eta^{(\prime)}, we show that B(Ξ›b→Λη, Λη′)=(1.47Β±0.35,1.83Β±0.58)Γ—10βˆ’6{\cal B}(\Lambda_b\to \Lambda\eta,\,\Lambda\eta^\prime)= (1.47\pm 0.35,1.83\pm 0.58)\times 10^{-6}, which are consistent with the current data of (9.3βˆ’5.3+7.3,<3.1)Γ—10βˆ’6(9.3^{+7.3}_{-5.3},<3.1)\times 10^{-6}, respectively. Our results also support the relation of B(Ξ›b→Λη)≃B(Ξ›b→Λη′){\cal B}(\Lambda_b\to \Lambda\eta) \simeq {\cal B}(\Lambda_b\to\Lambda\eta^\prime), given by the previous study.Comment: 8 pages, 1 figure, revised version accepted by EPJ

    The capacity region of classes of product broadcast channels

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    We establish a new outer bound for the capacity region of product broadcast channels. This outer bound matches Marton's inner bound for a variety of classes of product broadcast channels whose capacity regions were previously unknown. These classes include product of reversely semi-deterministic and product of reversely more-capable channels. A significant consequence of this new outer bound is that it establishes, via an example, that the previously best known outer-bound is strictly suboptimal for the general broadcast channel. Our example is comprised of a product broadcast channel with two semi-deterministic components in reverse orientation.Comment: full version of isit pape
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