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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 $D^+to K^0_SK^0_S K^+$, $D^+to K^0_SK^0_S pi^+$, $D^0to K^0_S K^0_S$ and $D^0to K^0_SK^0_SK^0_S$. They are determined to be ${mathcal B}(D^+to K^0_SK^0_SK^+)=(2.54 pm 0.05_{rm stat.} pm 0.12_{rm sys.})times 10^{-3}$, ${mathcal B}(D^+to K^0_SK^0_Spi^+)=(2.70 pm 0.05_{rm stat.} pm 0.12_{rm sys.})times 10^{-3}$, ${mathcal B}(D^0to K^0_SK^0_S)=(1.67 pm 0.11_{rm stat.} pm 0.11_{rm sys.})times 10^{-4}$ and ${mathcal B}(D^0to K^0_SK^0_SK^0_S)=(7.21 pm 0.33_{rm stat.} pm 0.44_{rm sys.})times 10^{-4}$, where the second one is measured for the first time and the others are measured with significantly improved precision over the previous measurements.
Analyzing $(448.1pm2.9)times10^6$ $psi(3686)$ events collected with the BESIII detector at the BEPCII collider, the $psi(3686)to omega K_{S}^{0}K_{S}^{0}$ decay is observed for the first time. The branching fraction for this decay is determined to be
We report a study of the decay $D^0 to K^0_S K^0_S$ using 921~fb$^{-1}$ of data collected at or near the $Upsilon(4S)$ and $Upsilon(5S)$ resonances with the Belle detector at the KEKB asymmetric energy $e^+e^-$ collider. The measured time-integrated
The first observation of the $B^0_stobar{D}^0 K^0_S$ decay mode and evidence for the $B^0_stobar{D}^{*0} K^0_S$ decay mode are reported. The data sample corresponds to an integrated luminosity of 3.0 $text{fb}^{-1}$ collected in $pp$ collisions by LH
Amplitude models are applied to studies of resonance structure in $D^0to K^0_S K^- pi^+$ and $D^0to K^0_S K^+ pi^-$ decays using $pp$ collision data corresponding to an integrated luminosity of $3.0,mathrm{fb}^{-1}$ collected by the LHCb experiment.