Measurements of the branching fractions for $D^+\to K^0_SK^0_SK^+$, $K^0_SK^0_S\pi^+$ and $D^0\to K^0_SK^0_S$, $K^0_SK^0_SK^0_S$

dc.contributor.authorMitchell, R. E., et al
dc.date.accessioned2025-02-20T15:48:57Z
dc.date.available2025-02-20T15:48:57Z
dc.date.issued2016-12-23
dc.description.abstractBy analyzing $2.93\ \rm fb^{-1}$ of data taken at the $\psi(3770)$ resonance peak with the BESIII detector, we measure the branching fractions for the hadronic decays $D^+\to K^0_SK^0_S K^+$, $D^+\to K^0_SK^0_S \pi^+$, $D^0\to K^0_S K^0_S$ and $D^0\to K^0_SK^0_SK^0_S$. They are determined to be ${\mathcal B}(D^+\to K^0_SK^0_SK^+)=(2.54 \pm 0.05_{\rm stat.} \pm 0.12_{\rm sys.})\times 10^{-3}$, ${\mathcal B}(D^+\to K^0_SK^0_S\pi^+)=(2.70 \pm 0.05_{\rm stat.} \pm 0.12_{\rm sys.})\times 10^{-3}$, ${\mathcal B}(D^0\to K^0_SK^0_S)=(1.67 \pm 0.11_{\rm stat.} \pm 0.11_{\rm sys.})\times 10^{-4}$ and ${\mathcal B}(D^0\to K^0_SK^0_SK^0_S)=(7.21 \pm 0.33_{\rm stat.} \pm 0.44_{\rm sys.})\times 10^{-4}$, where the second one is measured for the first time and the others are measured with significantly improved precision over the previous measurements.
dc.identifier.citationMitchell, R. E., et al. "Measurements of the branching fractions for $D^+\to K^0_SK^0_SK^+$, $K^0_SK^0_S\pi^+$ and $D^0\to K^0_SK^0_S$, $K^0_SK^0_SK^0_S$." Phys. Lett., vol. B765, pp. 231-237, 2016-12-23, https://doi.org/10.1016/j.physletb.2016.12.020.
dc.identifier.issn0031-9163
dc.identifier.otherBRITE 1005
dc.identifier.urihttps://hdl.handle.net/2022/31110
dc.language.isoen
dc.relation.isversionofhttps://doi.org/10.1016/j.physletb.2016.12.020
dc.relation.isversionofhttps://doi.org/10.1016/j.physletb.2016.12.020
dc.relation.journalPhys. Lett.
dc.titleMeasurements of the branching fractions for $D^+\to K^0_SK^0_SK^+$, $K^0_SK^0_S\pi^+$ and $D^0\to K^0_SK^0_S$, $K^0_SK^0_SK^0_S$

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