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arXiv:2412.10677·v1·High Energy Physics — Experiment

Observations of the singly Cabibbo-suppressed decays , , and at Belle and Belle II

Belle · Belle II Collaborations: I. Adachi · L. Aggarwal · N. Akopov · M. Alhakami · A. Aloisio · N. Althubiti · N. Anh Ky · D. M. Asner · H. Atmacan · T. Aushev · V. Aushev

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Abstract

Using data samples of 983.0~ and 427.9~ accumulated with the Belle and Belle~II detectors operating at the KEKB and SuperKEKB asymmetric-energy colliders, singly Cabibbo-suppressed decays , , and are observed for the first time. The ratios of branching fractions of , , and relative to that of are measured to be \begin{equation} \frac{{\cal B}(\Xi_c^+ \to pK_S^0)}{{\cal B}(\Xi_c^{+} \to \Xi^{-} \pi^+ \pi^+)} = (2.47 \pm 0.16 \pm 0.07)\% \notag, \end{equation} \begin{equation} \frac{{\cal B}(\Xi_c^+ \to \Lambda \pi^+)}{{\cal B}(\Xi_c^{+} \to \Xi^{-} \pi^+ \pi^+)} = (1.56 \pm 0.14 \pm 0.09)\% \notag, \end{equation} \begin{equation} \frac{{\cal B}(\Xi_c^+ \to \Sigma^0 \pi^+)}{{\cal B}(\Xi_c^{+} \to \Xi^{-} \pi^+ \pi^+)} = (4.13 \pm 0.26 \pm 0.22)\% \notag. \end{equation} Multiplying these values by the branching fraction of the normalization channel, , the absolute branching fractions are determined to be \begin{equation} {\cal B}(\Xi_c^{+} \to p K_{S}^{0}) = (7.16 \pm 0.46 \pm 0.20 \pm 3.21) \times 10^{-4} \notag, \end{equation} \begin{equation} {\cal B}(\Xi_c^{+} \to \Lambda \pi^+) = (4.52 \pm 0.41 \pm 0.26 \pm 2.03) \times 10^{-4} \notag, \end{equation} \begin{equation} {\cal B}(\Xi_c^{+} \to \Sigma^0 \pi^+) = (1.20 \pm 0.08 \pm 0.07 \pm 0.54) \times 10^{-3} \notag. \end{equation} The first and second uncertainties above are statistical and systematic, respectively, while the third ones arise from the uncertainty in .

Comments: 21 pages, 5 pages

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