TY - JOUR
T1 - Study of the semileptonic decay D0→K¯0π−e+νe
AU - Ablikim, M.
AU - Achasov, M. N.
AU - Adlarson, P.
AU - Afedulidis, O.
AU - Kabana, S.
AU - The BESIII collaboration
N1 - Publisher Copyright:
© The Author(s) 2025.
PY - 2025/3
Y1 - 2025/3
N2 - We report an improved study of the semileptonic decay D0→K¯0π−e+νe based on a sample of 7.9 fb−1 of e+e− annihilation data collected at a center-of-mass energy of 3.773 GeV with the BESIII detector at the BEPCII collider. The branching fraction of this decay is measured to be BD0→K¯0π−e+νe = (1.444 ± 0.022stat ± 0.024syst)%, which is the most precise to date, where the first uncertainty is statistical and the second is systematic. Based on investigation of the decay dynamics, we find that the decay is dominated by the K*(892)− component and present an improved measurement of its branching fraction to be BD0→K∗892−e+νe = (2.039 ± 0.032stat± 0.034syst)%. We also determine the ratios of the hadronic form factors for the K*(892)−e+νe decay to be rV = V(0)/A1(0) = 1.48 ± 0.05stat± 0.02syst and r2 = A2(0)/A1(0) = 0.70 ± 0.04stat± 0.02syst, where V(0) is the vector form factor and A1,2(0) are the axial form factors. In addition, the K¯0π−S-wave component is found to account for (5.87 ± 0.32stat± 0.16syst)% of the total decay rate, corresponding to a branching fraction of BD0→K¯0π−S−wavee+νe = (0.085 ± 0.005stat± 0.003syst)%.
AB - We report an improved study of the semileptonic decay D0→K¯0π−e+νe based on a sample of 7.9 fb−1 of e+e− annihilation data collected at a center-of-mass energy of 3.773 GeV with the BESIII detector at the BEPCII collider. The branching fraction of this decay is measured to be BD0→K¯0π−e+νe = (1.444 ± 0.022stat ± 0.024syst)%, which is the most precise to date, where the first uncertainty is statistical and the second is systematic. Based on investigation of the decay dynamics, we find that the decay is dominated by the K*(892)− component and present an improved measurement of its branching fraction to be BD0→K∗892−e+νe = (2.039 ± 0.032stat± 0.034syst)%. We also determine the ratios of the hadronic form factors for the K*(892)−e+νe decay to be rV = V(0)/A1(0) = 1.48 ± 0.05stat± 0.02syst and r2 = A2(0)/A1(0) = 0.70 ± 0.04stat± 0.02syst, where V(0) is the vector form factor and A1,2(0) are the axial form factors. In addition, the K¯0π−S-wave component is found to account for (5.87 ± 0.32stat± 0.16syst)% of the total decay rate, corresponding to a branching fraction of BD0→K¯0π−S−wavee+νe = (0.085 ± 0.005stat± 0.003syst)%.
KW - Charm Physics
KW - e-e Experiments
UR - https://www.scopus.com/pages/publications/105002023770
U2 - 10.1007/JHEP03(2025)197
DO - 10.1007/JHEP03(2025)197
M3 - Article
AN - SCOPUS:105002023770
SN - 1126-6708
VL - 2025
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 3
M1 - 197
ER -