Abstract
The four-body non-resonant rare \(\bar{B}\rightarrow \bar{K}\pi \ell \ell \) decay is important both as a background to the benchmark resonant mode \(\bar{B}\rightarrow \bar{K}^*\ell \ell \) and as sensitive probe for new physics beyond the Standard Model (SM). We show that in the SM the branching ratio of \(\bar{B}\rightarrow \bar{K}\pi \ell \ell \) is of the order few \(10^{-8}\), which is only an order of magnitude smaller than the \(\bar{B}\rightarrow \bar{K}^*\ell \ell \) decay. Nevertheless, the non-resonant mode is the dominant background to \(\bar{B}\rightarrow \bar{K}^*\ell \ell \) compared to other low mass scalars. We study the angular distributions of the non-resonant mode and show that the decay offers new combinations of short-distance couplings that are absent in the resonant decay. We explore interesting phenomenology in the interference of the resonant and non-resonant modes and discuss methods to extract the relative strong phase. The new physics sensitivity in the light of interference is also discussed.
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Acknowledgements
The author would like to thank the organizers of pheno1@IISERM for organizing a wonderful workshop at IISER Mohali and for giving him the opportunity to present the work. The author would also like to thank Gudrun Hiller, Martin Jung and Alex Shires for fruitful collaborations.
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Das, D. The \(B\rightarrow \bar{K}\pi \ell \ell \) distribution at low hadronic recoil. Pramana - J Phys 89, 61 (2017). https://doi.org/10.1007/s12043-017-1455-3
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DOI: https://doi.org/10.1007/s12043-017-1455-3