Abstract
We report a study of the decay $D^0 \rightarrow \bar{K}^0\pi^-e^+\nu_{e}$ based on a sample of $2.93~\mathrm{fb}^{-1}$ $e^+e^-$ annihilation data collected at the center-of-mass energy of 3.773~GeV with the BESIII detector at the BEPCII collider. The total branching fraction is determined to be $\mathcal{B}(D^0\rightarrow \bar{K}^0\pi^-e^+\nu_{e})=(1.434\pm0.029({\rm stat.})\pm0.032({\rm syst.}))\%$, which is the most precise to date. According to a detailed analysis of the involved dynamics, we find this decay is dominated with the $K^{*}(892)^-$ contribution and present an improved measurement of its branching fraction to be $\mathcal{B}(D^0\rightarrow K^{*}(892)^-e^+\nu_e)=(2.033\pm0.046({\rm stat.})\pm0.047({\rm syst.}))\%$. We further access their hadronic form-factor ratios for the first time as $r_{V}=V(0)/A_1(0)=1.46\pm0.07({\rm stat.})\pm0.02({\rm syst.})$ and $r_{2}=A_2(0)/A_1(0)=0.67\pm0.06({\rm stat.})\pm0.01({\rm syst.})$. In addition, we observe a significant $\bar{K}^0\pi^-$ $S$-wave component accounting for $(5.51\pm0.97({\rm stat.})\pm0.62({\rm syst.}))\%$ of the total decay rate.
Highlights
strong interactions in mesons composed of heavy quarks
The semileptonic partial decay width is related to the product of the hadronic form factor describing the stronginteraction
which parametrize the mixing between the quark flavors in the weak interaction
Summary
The studies on semileptonic (SL) decay modes of charm mesons provide valuable information on the weak and strong interactions in mesons composed of heavy quarks [1]. Detailed studies of the dynamics of the SL decays allow measurements of the hadronic form factors, which are important for calibrating the theoretical calculations of the involved strong interaction. An improved measurement of the absolute branching fraction (BF) and the first measurement of the form factors of the decay D0 → K 0π−eþνe are reported. These measurements are performed using an eþe− annihniolsaittiyonofd2a.t9a3safmb−p1leprcoodrurecsepdoantdpinffisgffi to 1⁄4. An integrated lumi3.773 GeV with the BEPCII collider and collected with the BESIII detector [9]
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