5,982 research outputs found

    Some Predictions of Diquark Model for Hidden Charm Pentaquark Discovered at the LHCb

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    The LHCb has discovered two new states with preferred JPJ^P quantum numbers 3/2βˆ’3/2^- and 5/2+5/2^+ from Ξ›b\Lambda_b decays. These new states can be interpreted as hidden charm pentaquarks. It has been argued that the main features of these pentaquarks can be described by diquark model. The diquark model predicts that the 3/2βˆ’3/2^- and 5/2+5/2^+ are in two separate octet multiplets of flavor SU(3)SU(3) and there is also an additional decuplet pentaquark multiplet. Finding the states in these multiplets can provide crucial evidence for this model. The weak decays of b-baryon to a light meson and a pentaquark can have Cabibbo allowed and suppressed decay channels. We find that in the SU(3)SU(3) limit, for UU-spin related decay modes the ratio of the decay rates of Cabibbo suppressed to Cabibbo allowed decay channels is given by ∣Vcd∣2/∣Vcs∣2|V_{cd}|^2/|V_{cs}|^2. There are also other testable relations for b-baryon weak decays into a pentaquark and a light pseudoscalar. These relations can be used as tests for the diquark model for pentaquark.Comment: revtex, 19 pages, 3 figures. one reference added and some typos correcte

    Predictive CPCP Violating Relations for Charmless Two-body Decays of Beauty Baryons Ξbβˆ’,β€…β€Š0\Xi^{-,\;0}_b and Ξ›b0\Lambda_b^0 With Flavor SU(3)SU(3) Symmetry

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    Several baryons containing a heavy b-quark have been discovered. The decays of these states provide new platform for testing the standard model (SM). We study CPCP violation in SM for charmless two-body decays of the flavor SU(3)SU(3) anti-triplet beauty baryon (b-baryon) B=(Ξbβˆ’,β€…β€ŠΞžb0,β€…β€ŠΞ›b0){\cal B} = (\Xi^-_b,\;\Xi^0_b,\;\Lambda_b^0) in a model independent way. We found, in the flavor SU(3)SU(3) symmetry limit, a set of new predictive relations among the branching ratio BrBr and CPCP asymmetry ACPA_{CP} for B\cal B decays, such as ACP(Ξbβˆ’β†’K0Ξžβˆ’)/ACP(Ξbβˆ’β†’KΛ‰0Ξ£βˆ’)=βˆ’Br(Ξbβˆ’β†’KΛ‰0Ξ£βˆ’)/Br(Ξbβˆ’β†’K0Ξ£βˆ’)A_{CP}(\Xi_b^-\to K^0 \Xi^-)/A_{CP}(\Xi_b^-\to \bar K^0 \Sigma^-) = - Br(\Xi_b^- \to \bar K^0 \Sigma^-)/Br(\Xi_b^- \to K^0 \Sigma^-), ACP(Ξ›b0β†’Ο€βˆ’p)/ACP(Ξb0β†’Kβˆ’Ξ£+)=βˆ’Br(Ξb0β†’Kβˆ’Ξ£+)τΛb0/Br(Ξ›b0β†’Ο€βˆ’p)Ο„Ξžb0A_{CP}(\Lambda_b^0 \to \pi^- p)/A_{CP} (\Xi^0_b \to K^- \Sigma^+) = -Br(\Xi^0_b \to K^- \Sigma^+)\tau_{\Lambda_b^0}/Br(\Lambda_b^0 \to \pi^- p)\tau_{\Xi^0_b},and ACP(Ξ›b0β†’Kβˆ’p)/ACP(Ξb0β†’Ο€βˆ’Ξ£+)=βˆ’Br(Ξb0β†’Ο€βˆ’Ξ£+)τΛb0/Br(Ξ›b0β†’Kβˆ’p)Ο„Ξžb0A_{CP}(\Lambda_b^0 \to K^- p)/ A_{CP} (\Xi^0_b \to \pi^- \Sigma^+) = -Br(\Xi^0_b \to \pi^- \Sigma^+)\tau_{\Lambda_b^0}/ Br(\Lambda_b^0 \to K^- p)\tau_{\Xi^0_b}. Future data from LHCb can test these relations and also other relations found.Comment: 13 pages, no figure, 6 tables, several missing terms in eq.11 are adde

    CP violation in neutrino mixing with Ξ΄=βˆ’Ο€/2\delta = -\pi/2 in A4A_4 Type-II seesaw model

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    We study a class of models for neutrino mass matrix in Type-II seesaw with A4A_4 family symmetry. The resulting neutrino mass matrix can be naturally made to respect a ΞΌβˆ’Ο„\mu-\tau exchange plus CP conjugate symmetry (GLS) with the CP violating phase Ξ΄\delta and the mixing angle ΞΈ23\theta_{23} predicted to be Β±Ο€/2\pm\pi/2 and Ο€/4\pi/4, respectively. When GLS is explicitly broken by complex Yukawa couplings, the model predictions for Ξ΄\delta and ΞΈ23\theta_{23} can be significantly modified. Should future experiments will indeed determine ΞΈ23\theta_{23} and Ξ΄CP\delta_{CP} away from the GLS limit values, one then had to consider models with broken GLS. We study several simple scenarios to show how the modifications arise when GLS is broken and how future experiments can test this class of models.Comment: 15 pages, 3 figures, minor errors corrected. Version appeared in Phys.Lett.B. arXiv admin note: text overlap with arXiv:1504.0156

    U-spin analysis of CP violation in Bβˆ’B^- decays into three charged light pseudoscalar mesons

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    We carry out a UU-spin symmetry analysis for CP violation in Bβˆ’B^- decays into three light Ο€βˆ’Ο€βˆ’Ο€+\pi^-\pi^-\pi^+, Ο€βˆ’Kβˆ’K+\pi^- K^-K^+, Kβˆ’Kβˆ’K+K^-K^-K^+ and Kβˆ’Ο€βˆ’Ο€+K^- \pi^-\pi^+ mesons. We clarify some subtle points in constructing decay amplitudes with U=0U=0 formed by the two negatively charged light mesons in the final states. UU-spin conserving momentum independent and momentum dependent decay amplitudes, and UU-spin violating decay amplitudes due to quark mass difference are constructed.Comment: RevTex 12 pages wit no figur

    Coverage Analysis of Relay Assisted Millimeter Wave Cellular Networks with Spatial Correlation

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    We propose a novel analytical framework for evaluating the coverage performance of a millimeter wave (mmWave) cellular network where idle user equipments (UEs) act as relays. In this network, the base station (BS) adopts either the direct mode to transmit to the destination UE, or the relay mode if the direct mode fails, where the BS transmits to the relay UE and then the relay UE transmits to the destination UE. To address the drastic rotational movements of destination UEs in practice, we propose to adopt selection combining at destination UEs. New expression is derived for the signal-to-interference-plus-noise ratio (SINR) coverage probability of the network. Using numerical results, we first demonstrate the accuracy of our new expression. Then we show that ignoring spatial correlation, which has been commonly adopted in the literature, leads to severe overestimation of the SINR coverage probability. Furthermore, we show that introducing relays into a mmWave cellular network vastly improves the coverage performance. In addition, we show that the optimal BS density maximizing the SINR coverage probability can be determined by using our analysis
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