Physicists nail down rare particle decay rates with new precision
Researchers have measured how charm particles called D_s+ decay into other particles with unprecedented accuracy, filling a critical gap in the Standard Model of physics. These measurements could help explain matter-antimatter imbalances and validate theoretical models that guide future particle detector design and high-energy physics research.
Originaltitel: Measurements of the branching fractions of semileptonic <em>D<sub>s</sub></em><sup>+</sup> decays via <em>e</em><sup>+</sup><em>e</em><sup>-</sup> → <em>D<sub>s</sub></em>*<sup>+</sup><em>D<sub>s</sub></em>*<sup>-</sup>
<p>We measure the absolute branching fractions of semileptonic D<sub>s</sub><sup>+</sup>, decays via the e<sup>+</sup>e<sup>-</sup> → D<sub>s</sub><sup>*+</sup>D<sub>s</sub><sup>*-</sup> process using e<sup>+</sup>e<sup>-</sup> collision data corresponding to an integrated luminosity of 10.64 fb<sup>-1</sup> collected by the BESIII detector at center-of-mass energies between 4237 and 4.699 GeV. The branching fractions are <em>B</em>(D<sub>s</sub><sup>+</sup> → ηe<sup>+</sup>ν<sub>e</sub>) = (2.35 ± 0.11<sub>stat</sub> ± 0.10<sub>syst</sub>)%, <em>B</em>(D<sub>s</sub><sup>+</sup> → η'e<sup>+</sup>ν<sub>e</sub>) = (0.82 ± 0.09<sub>stat</sub> ± 0.04<sub>syst</sub>)%, <em>B</em>(D<sub>s</sub><sup>+</sup> → Φe<sup>+</sup>ν<sub>e</sub>) = (2.21 ± 0.16<sub>stat</sub> ± 0.11<sub>syst</sub>)%, <em>B</em>(D<sub>s</sub><sup>+</sup> → f(0)(980)e<sup>+</sup>ν<sub>e</sub>), f(0)(980) → π<sup>+</sup>π<sup>-</sup>) = (0.15 ± 0.02<sub>stat</sub> ± 0.01<sub>syst</sub>)%, <em>B</em>(D<sub>s</sub><sup>+</sup> → K<sup>0</sup>e<sup>+</sup>ν<sub>e</sub>) = (0.24 ± 0.04<sub>stat</sub> ± 0.01<sub>syst</sub>)%, and <em>B</em>(D<sub>s</sub><sup>+</sup> → K<sup>0</sup>e<sup>+</sup>ν<sub>e</sub>) = (0.19 ± 0.03<sub>stat</sub> ± 0.01<sub>syst</sub>)%. These results are consistent with those measured via the e<sup>+</sup>e<sup>- </sup>→ D<sub>s</sub><sup>*+/-</sup>D<sub>s</sub><sup>-/+</sup> process by BESIII and CLEO. Using two -parameter series expansion, the hadronic transition form factors of D<sub>s</sub><sup>+</sup> → ηe<sup>+</sup>ν<sub>e</sub>, D<sub>s</sub><sup>+</sup> → η'e<sup>+</sup>ν<sub>e</sub> and D<sub>s</sub><sup>+</sup> → K<sup>0</sup>e<sup>+</sup>ν<sub>e</sub> are determined to be f<sub>+</sub><sup>η</sup>(0) = 0.442 ± 0.022<sub>stat </sub>± 0.017<sub>syst</sub>, f<sub>+</sub><sup>η'</sup>(0) = 0.557 ± 0.062<sub>stat</sub> ± 0.024<sub>syst</sub>, and f<sub>+</sub><sup>K^0</sup>(0) = 0.677 ± 0.098<sub>stat</sub> ± 0.023<sub>syst</sub>.</p>