3,908 research outputs found

    Localized direct CP violation in B±→ρ0(Ο‰)π±→π+Ο€βˆ’Ο€Β±B^\pm\rightarrow \rho^0 (\omega)\pi^\pm\rightarrow \pi^+ \pi^-\pi^\pm

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    We study the localized direct CP violation in the hadronic decays B±→ρ0(Ο‰)π±→π+Ο€βˆ’Ο€Β±B^\pm\rightarrow \rho^0 (\omega)\pi^\pm\rightarrow\pi^+ \pi^-\pi^\pm, including the effect caused by an interesting mechanism involving the charge symmetry violating mixing between ρ0\rho^0 and Ο‰\omega. We calculate the localized integrated direct CP violation when the low invariant mass of Ο€+Ο€βˆ’\pi^+\pi^- [m(Ο€+Ο€βˆ’)lowm(\pi^+\pi^-)_{low}] is near ρ0(770)\rho^0(770). For five models of form factors investigated, we find that the localized integrated direct CP violation varies from -0.0170 to -0.0860 in the ranges of parameters in our model when 0.750<m(Ο€+Ο€βˆ’)low<0.8000.750<m(\pi^+\pi^-)_{low}<0.800\,GeV. This result, especially the sign, agrees with the experimental data and is independent of form factor models. The new experimental data shows that the signs of the localized integrated CP asymmetries in the regions 0.470<m(Ο€+Ο€βˆ’)low<0.7700.470<m(\pi^+\pi^-)_{low}<0.770\,GeV and 0.770<m(Ο€+Ο€βˆ’)low<0.9200.770<m(\pi^+\pi^-)_{low}<0.920\,GeV are positive and negative, respectively. We find that ρ\rho-Ο‰\omega mixing makes the localized integrated CP asymmetry move towards the negative direction, and therefore contributes to the sign change in those two regions. This behavior is also model independent. We also calculate the localized integrated direct CP violating asymmetries in the regions 0.470<m(Ο€+Ο€βˆ’)low<0.7700.470<m(\pi^+\pi^-)_{low}<0.770\,GeV and 0.770<m(Ο€+Ο€βˆ’)low<0.9200.770<m(\pi^+\pi^-)_{low}<0.920\,GeV and find that they agree with the experimental data in some models of form factors.Comment: 22 pages, 2 figures. arXiv admin note: text overlap with arXiv:hep-ph/0602043, arXiv:hep-ph/0302156 by other author

    Kernel Truncated Regression Representation for Robust Subspace Clustering

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    Subspace clustering aims to group data points into multiple clusters of which each corresponds to one subspace. Most existing subspace clustering approaches assume that input data lie on linear subspaces. In practice, however, this assumption usually does not hold. To achieve nonlinear subspace clustering, we propose a novel method, called kernel truncated regression representation. Our method consists of the following four steps: 1) projecting the input data into a hidden space, where each data point can be linearly represented by other data points; 2) calculating the linear representation coefficients of the data representations in the hidden space; 3) truncating the trivial coefficients to achieve robustness and block-diagonality; and 4) executing the graph cutting operation on the coefficient matrix by solving a graph Laplacian problem. Our method has the advantages of a closed-form solution and the capacity of clustering data points that lie on nonlinear subspaces. The first advantage makes our method efficient in handling large-scale datasets, and the second one enables the proposed method to conquer the nonlinear subspace clustering challenge. Extensive experiments on six benchmarks demonstrate the effectiveness and the efficiency of the proposed method in comparison with current state-of-the-art approaches.Comment: 14 page

    Possible large CPCP violation in three body decays of heavy baryon

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    We propose a new mechanism which can introduce large CPCP asymmetries in the phase spaces of three-body decays of heavy baryons. In this mechanism, a large CPCP asymmetry is induced by the interference of two intermediate resonances, which subsequently decay into two different combinations of final particles. We apply this mechanism to the decay channel Ξ›b0β†’pΟ€0Ο€βˆ’\Lambda_b^0 \to p \pi^0\pi^-, and find that the differential CPCP asymmetry can reach as large as 50%50\%, while the regional CPCP asymmetry can reach as large as 16%16\% in the interference region of the phase space.Comment: 7 pages, 2 figures, 2nd version accepted by Phys. Lett.
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