Study of the decay $D^0\rightarrow \bar{K}^0\pi^-e^+\nu_e$
dc.contributor.author | Ablikim, M. | |
dc.contributor.author | Mitchell, R. E., et al | |
dc.date.accessioned | 2025-02-20T16:16:53Z | |
dc.date.available | 2025-02-20T16:16:53Z | |
dc.date.issued | 2019-01-25 | |
dc.description.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 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. | |
dc.identifier.citation | Ablikim, M., and Mitchell, R. E., et al. "Study of the decay $D^0\rightarrow \bar{K}^0\pi^-e^+\nu_e$." Physical Review D, vol. D99, no. 1, 2019-01-25, https://doi.org/10.1103/PhysRevD.99.011103. | |
dc.identifier.issn | 2470-0010 | |
dc.identifier.other | BRITE 6230 | |
dc.identifier.uri | https://hdl.handle.net/2022/31864 | |
dc.language.iso | en | |
dc.relation.isversionof | https://doi.org/10.1103/PhysRevD.99.011103 | |
dc.relation.isversionof | https://journals.aps.org/prd/abstract/10.1103/PhysRevD.99.011103 | |
dc.relation.journal | Physical Review D | |
dc.title | Study of the decay $D^0\rightarrow \bar{K}^0\pi^-e^+\nu_e$ |
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