19,654 research outputs found

    Branching ratios and CPCP asymmetries of B→χc1K(π)B\rightarrow \chi_{c1}K(\pi) decays

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    We investigate the exclusive nonleptonic decays Bβ†’Ο‡c1K(Ο€)B\rightarrow \chi_{c1}K(\pi) in the conventional perturbative QCD (PQCD) formalism. The predictions of branching ratios and CPCP asymmetries are given in detail. We compare our results with available experimental data as well as predictions of other theoretical studies existing in the literature. It seems that the branching ratios of Bβ†’Ο‡c1KB\rightarrow \chi_{c1} K are more consistent with data than the earlier analyses. For the Cabibbo-suppressed BsB_s decay, the branching ratio can reach the order of 10βˆ’510^{-5}, which would be straight forward for experimental observations. The numerical results show that the direct CPCP asymmetries of the concerned decays are rather small. The mixing-induced CPCP asymmetry in the B0β†’Ο‡c1KSB^0\rightarrow \chi_{c1}K_S is very close to sin⁑2Ξ²\sin{2\beta}, which suggests that this channel offer an alternative method for measuring the Cabbibo-Kobayashi-Maskawa (CKM) angle Ξ²\beta. The obtained results in the present work could be tested by further experiments in the LHCb and forthcoming Belle II.Comment: 8 pages, 1 figur

    Facility location with double-peaked preference

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    We study the problem of locating a single facility on a real line based on the reports of self-interested agents, when agents have double-peaked preferences, with the peaks being on opposite sides of their locations. We observe that double-peaked preferences capture real-life scenarios and thus complement the well-studied notion of single-peaked preferences. We mainly focus on the case where peaks are equidistant from the agents' locations and discuss how our results extend to more general settings. We show that most of the results for single-peaked preferences do not directly apply to this setting; this makes the problem essentially more challenging. As our main contribution, we present a simple truthful-in-expectation mechanism that achieves an approximation ratio of 1+b/c for both the social and the maximum cost, where b is the distance of the agent from the peak and c is the minimum cost of an agent. For the latter case, we provide a 3/2 lower bound on the approximation ratio of any truthful-in-expectation mechanism. We also study deterministic mechanisms under some natural conditions, proving lower bounds and approximation guarantees. We prove that among a large class of reasonable mechanisms, there is no deterministic mechanism that outperforms our truthful-in-expectation mechanism

    Ξ›bβ†’Ξ›cτνˉτ\Lambda_b\to\Lambda_c\tau\bar\nu_\tau decay in scalar and vector leptoquark scenarios

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    It has been shown that the anomalies observed in BΛ‰β†’D(βˆ—)τνˉτ\bar B\to D^{(\ast)}\tau\bar\nu_\tau and BΛ‰β†’KΛ‰β„“+β„“βˆ’\bar B\to \bar K\ell^+\ell^- decays can be resolved by adding a single scalar or vector leptoquark to the Standard Model, while constraints from other precision measurements in the flavour sector can be satisfied without fine-tuning. To further explore these two interesting scenarios, in this paper, we study their effects in the semi-leptonic Ξ›bβ†’Ξ›cτνˉτ\Lambda_b\to\Lambda_c\tau\bar\nu_\tau decay. Using the best-fit solutions for the operator coefficients allowed by the current data of mesonic decays, we find that (i) the two scenarios give similar amounts of enhancements to the branching fraction B(Ξ›bβ†’Ξ›cτνˉτ)\mathcal B(\Lambda_b\to\Lambda_c\tau\bar\nu_\tau) and the ratio RΞ›c=B(Ξ›bβ†’Ξ›cτνˉτ)/B(Ξ›bβ†’Ξ›cβ„“Ξ½Λ‰β„“)R_{\Lambda_c}=\mathcal B(\Lambda_b\to\Lambda_c \tau\bar\nu_\tau)/\mathcal B(\Lambda_b\to\Lambda_c\ell\bar\nu_\ell), (ii) the two best-fit solutions in each of these two scenarios are also indistinguishable from each other, (iii) both scenarios give nearly the same predictions as those of the Standard Model for the longitudinal polarizations of Ξ›c\Lambda_c and Ο„\tau as well as the lepton-side forward-backward asymmetry. With future measurements of these observables in Ξ›bβ†’Ξ›cτνˉτ\Lambda_b\to\Lambda_c\tau\bar\nu_\tau decay at the LHCb, the two leptoquark scenarios could be further tested, and even differentiated from the other NP explanations for the RD(βˆ—)R_{D^{(\ast)}} anomalies. We also discuss the feasibility for the measurements of these observables at the LHC and the future e+eβˆ’e^+e^- colliders.Comment: 29 pages, 4 tables and 2 figures; More references and the feasibility for the measurements of the observables in these decays at the LHC and the future e+eβˆ’e^+e^- colliders added, final version published in the journa
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