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.author | Mitchell, R. E., et al | |
dc.date.accessioned | 2025-02-20T15:48:57Z | |
dc.date.available | 2025-02-20T15:48:57Z | |
dc.date.issued | 2016-12-23 | |
dc.description.abstract | By 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.citation | Mitchell, 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.issn | 0031-9163 | |
dc.identifier.other | BRITE 1005 | |
dc.identifier.uri | https://hdl.handle.net/2022/31110 | |
dc.language.iso | en | |
dc.relation.isversionof | https://doi.org/10.1016/j.physletb.2016.12.020 | |
dc.relation.isversionof | https://doi.org/10.1016/j.physletb.2016.12.020 | |
dc.relation.journal | Phys. Lett. | |
dc.title | Measurements of the branching fractions for $D^+\to K^0_SK^0_SK^+$, $K^0_SK^0_S\pi^+$ and $D^0\to K^0_SK^0_S$, $K^0_SK^0_SK^0_S$ |
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