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    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 Λb0pπ0π\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.

    Localized direct CP violation in B±ρ0(ω)π±π+ππ±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(ω)π±π+ππ±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 ω\omega. We calculate the localized integrated direct CP violation when the low invariant mass of π+π\pi^+\pi^- [m(π+π)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(π+π)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(π+π)low<0.7700.470<m(\pi^+\pi^-)_{low}<0.770\,GeV and 0.770<m(π+π)low<0.9200.770<m(\pi^+\pi^-)_{low}<0.920\,GeV are positive and negative, respectively. We find that ρ\rho-ω\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(π+π)low<0.7700.470<m(\pi^+\pi^-)_{low}<0.770\,GeV and 0.770<m(π+π)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

    2-(4-Fluoro­phen­yl)-4-(4-meth­oxy­phen­yl)-5-(piperidin-1-ylmeth­yl)thia­zole

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    In the title compound, C22H23FN2OS, the piperidine ring shows chair confirmation and the two benzene rings make a dihedral angle of 17.0 (6)°. The thia­zole fragment is essentially planar with an r.m.s. deviation of 0.004 (2) Å and a maximum deviation of 0.006 (2) Å.. In the crystal, inter­molecular C—H⋯π inter­actions lead to the formation of a layer structure
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