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Institute of High Energy Physics, Beijing 100049, People's Republic of China.
G.I. Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russia.
Phys Rev Lett. 2021 Oct 22;127(17):171801. doi: 10.1103/PhysRevLett.127.171801.
Using a dataset of 6.32 fb^{-1} of e^{+}e^{-} annihilation data collected with the BESIII detector at center-of-mass energies between 4178 and 4226 MeV, we have measured the absolute branching fraction of the leptonic decay D_{s}^{+}→τ^{+}ν_{τ} via τ^{+}→e^{+}ν_{e}ν[over ¯]{τ}, and find B{D_{s}^{+}→τ^{+}ν_{τ}}=(5.27±0.10±0.12)×10^{-2}, where the first uncertainty is statistical and the second is systematic. The precision is improved by a factor of 2 compared to the previous best measurement. Combining with f_{D_{s}^{+}} from lattice quantum chromodynamics calculations or the |V_{cs}| from the CKMfitter group, we extract |V_{cs}|=0.978±0.009±0.012 and f_{D_{s}^{+}}=(251.1±2.4±3.0) MeV, respectively. Combining our result with the world averages of B_{D_{s}^{+}→τ^{+}ν_{τ}} and B_{D_{s}^{+}→μ^{+}ν_{μ}}, we obtain the ratio of the branching fractions B_{D_{s}^{+}→τ^{+}ν_{τ}}/B_{D_{s}^{+}→μ^{+}ν_{μ}}=9.72±0.37, which is consistent with the standard model prediction of lepton flavor universality.
利用北京谱仪III(BESIII)探测器在质心能量为4178至4226兆电子伏特之间收集的6.32飞靶^{-1}的正负电子对撞数据,我们通过τ^{+}→e^{+}ν_{e}ν[上划线]{τ}测量了轻子衰变D{s}^{+}→τ^{+}ν_{τ} 的绝对分支比,结果为B_{D_{s}^{+}→τ^{+}ν_{τ}}=(5.27±0.10±0.12)×10^{-2},其中第一个不确定度为统计不确定度,第二个为系统不确定度。与之前的最佳测量结果相比,精度提高了一倍。结合格点量子色动力学计算得到的f_{D_{s}^{+}}或CKMfitter组得到的|V_{cs}|,我们分别提取出|V_{cs}|=0.978±0.009±0.012和f_{D_{s}^{+}}=(251.1±2.4±3.0)兆电子伏特。将我们的结果与D_{s}^{+}→τ^{+}ν_{τ}和D_{s}^{+}→μ^{+}ν_{μ}的世界平均值相结合,我们得到分支比的比值B_{D_{s}^{+}→τ^{+}ν_{τ}}/B_{D_{s}^{+}→μ^{+}ν_{μ}}=9.72±0.37,这与轻子味普适性的标准模型预测一致。