Direct CP violation in internal W-emission dominated baryonic B decays

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Y. K. Hsiao
Shang-Yuu Tsai
Eduardo Rodrigues
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[1] Shanxi Normal University,School of Physics and Information Engineering
[2] University of Liverpool,Oliver Lodge Laboratory
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The observation of CP violation has been experimentally verified in numerous B decays but is yet to be confirmed in final states with half-spin particles. We focus our attention on baryonic B-meson decays mediated dominantly through internal W-emission processes and show that they are promising processes to observe for the first time the CP violating effects in B decays to final states with half-spin particles. Specifically, we study the B¯0→pp¯π0(ρ0)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\bar{B}^0\rightarrow p\bar{p}\pi ^0(\rho ^0)$$\end{document} and B¯0→pp¯π+π-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\bar{B}^0\rightarrow p\bar{p}\pi ^+\pi ^-$$\end{document} decays. We obtain B(B¯0→pp¯π0)=(5.0±2.1)×10-7\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{B}(\bar{B}^0\rightarrow p\bar{p}\pi ^0)=(5.0\pm 2.1)\times 10^{-7}$$\end{document}, in agreement with current data, and B(B¯0→pp¯ρ0)≃B(B¯0→pp¯π0)/3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{B}(\bar{B}^0\rightarrow p\bar{p}\rho ^0)\simeq \mathcal{B}(\bar{B}^0\rightarrow p\bar{p}\pi ^0)/3$$\end{document}. Furthermore, we find ACP(B¯0→pp¯π0,pp¯ρ0,pp¯π+π-)=(-16.8±5.4,-12.6±3.0,-11.4±1.9)%\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{A}_{CP}(\bar{B}^0\rightarrow p\bar{p}\pi ^0,p\bar{p}\rho ^0,p\bar{p}\pi ^+\pi ^-) =(-16.8\pm 5.4,-12.6\pm 3.0,-11.4\pm 1.9)\%$$\end{document}. With measured branching fractions B(B¯0→pp¯π0,pp¯π+π-)∼O(10-6)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{B}(\bar{B}^0\rightarrow p\bar{p}\pi ^0,p\bar{p}\pi ^+\pi ^-)\sim \mathcal{O}(10^{-6})$$\end{document}, we point out that ACP∼-(10-20)%\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{A}_{CP}\sim -(10-20)\%$$\end{document} can be new observables for CP violation, accessible to the Belle II and/or LHCb experiments.
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