1,424 research outputs found

    CP violation in neutrino mixing with δ=−Ī€/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 Îŧ−Ī„\mu-\tau exchange plus CP conjugate symmetry (GLS) with the CP violating phase δ\delta and the mixing angle θ23\theta_{23} predicted to be ÂąĪ€/2\pm\pi/2 and Ī€/4\pi/4, respectively. When GLS is explicitly broken by complex Yukawa couplings, the model predictions for δ\delta and θ23\theta_{23} can be significantly modified. Should future experiments will indeed determine θ23\theta_{23} and δCP\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

    Predictive CPCP Violating Relations for Charmless Two-body Decays of Beauty Baryons Ξb−,  0\Xi^{-,\;0}_b and Λb0\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=(Ξb−,  Ξb0,  Λb0){\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(Ξb−→K0Ξ−)/ACP(Ξb−→Kˉ0ÎŖ−)=−Br(Ξb−→Kˉ0ÎŖ−)/Br(Ξb−→K0ÎŖ−)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(Λb0→Ī€âˆ’p)/ACP(Ξb0→K−ÎŖ+)=−Br(Ξb0→K−ÎŖ+)Ī„Λb0/Br(Λb0→Ī€âˆ’p)Ī„Ξb0A_{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(Λb0→K−p)/ACP(Ξb0→Ī€âˆ’ÎŖ+)=−Br(Ξb0→Ī€âˆ’ÎŖ+)Ī„Λb0/Br(Λb0→K−p)Ī„Ξb0A_{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

    PENINJAUAN NEGASI DARI SEGI LINGUISTIK KOGNITIF (äģŽčŽ¤įŸĨ角åēĻįœ‹åĻ厚)

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    This paper makes a tentative attempt to the study of negation from a cognitive perspective. Mainly such aspects as the prototype and its category, the relation of figure and ground, and the iconicity are dealt with. The paper shows that a cognitive approach to the study negation may broaden the understanding of the areas studied by the conventional theories, and will further our comprehension of how language conceptualize the external world and of the underlying relationship between language and cognition

    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 3/2−3/2^- and 5/2+5/2^+ from Λb\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 3/2−3/2^- 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 âˆŖVcdâˆŖ2/âˆŖVcsâˆŖ2|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

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

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    We carry out a UU-spin symmetry analysis for CP violation in B−B^- decays into three light Ī€âˆ’Ī€âˆ’Ī€+\pi^-\pi^-\pi^+, Ī€âˆ’K−K+\pi^- K^-K^+, K−K−K+K^-K^-K^+ and K−Ī€âˆ’Ī€+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
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