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Study of the semileptonic decay D0→K¯0π−e+νe

  • BESIII Collaboration
  • CAS - Institute of High Energy Physics
  • Budker Institute of Nuclear Physics of the Siberian Branch of the RAS
  • Novosibirsk State University
  • Uppsala University
  • Ruhr University Bochum
  • Chinese Academy of Sciences
  • Zhengzhou University
  • Johannes Gutenberg University Mainz
  • University of Turin
  • National Institute for Nuclear Physics
  • Southeast University, Nanjing
  • Joint Institute for Nuclear Research
  • Peking University
  • University of Chinese Academy of Sciences
  • National Centre for Nuclear Research
  • Mongolian Academy of Sciences
  • Carnegie Mellon University
  • University of Münster
  • Wuhan University
  • University of Science and Technology of China
  • Istinye University
  • Nankai University
  • Moscow Institute of Physics and Technology
  • China University of Geosciences, Wuhan
  • Soochow University
  • Henan University
  • Nanjing University
  • North China Electric Power University
  • Tsinghua University
  • CAS - Institute of Modern Physics
  • Jilin University
  • Hunan University
  • Chung-Ang University
  • Shandong University
  • Yunnan University
  • Helmholtz Institute Mainz
  • University of South China
  • University of Jinan
  • Liaoning University
  • Henan Normal University
  • Sun Yat-Sen University
  • University of Eastern Piedmont
  • Nanjing Normal University
  • University of Ferrara
  • University of Manchester
  • University of Oxford
  • GSI Helmholtz Centre for Heavy Ion Research
  • Guangxi University
  • Shandong Normal University
  • Fudan University
  • Indiana University Bloomington
  • University of Hawai'i at Mānoa
  • Suranaree University of Technology
  • South China Normal University
  • University of the Punjab
  • Liaoning Normal University
  • Hangzhou Normal University
  • Huangshan College
  • University of Groningen
  • Indian Institute of Technology Madras
  • Justus Liebig University Giessen
  • Qufu Normal University
  • Renmin University of China
  • Lanzhou University
  • Hebei University
  • China Center of Advanced Science and Technology World Laboratory
  • Sichuan University
  • Guangxi Normal University
  • Shanxi University
  • Central China Normal University
  • Henan University of Science and Technology
  • Henan University of Technology
  • Central South University
  • Zhejiang University
  • Goethe University Frankfurt
  • COMSATS University Islamabad
  • IBA
  • University of Perugia
  • Universidad de Tarapacá
  • Petersburg Nuclear Physics Institute (PNPI)
  • Hunan Normal University
  • Swiss Federal Institute of Technology Lausanne
  • Shanghai Jiao Tong University
  • Ministry of Education of the People's Republic of China
  • Near East University
  • Inner Mongolia University
  • Yantai University
  • Beihang University
  • University of Bristol
  • Shanxi Normal University
  • University of Science and Technology Liaoning

Producción científica: Contribución a una revistaArtículorevisión exhaustiva

7 Citas (Scopus)

Resumen

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)%.

Idioma originalInglés
Número de artículo197
PublicaciónJournal of High Energy Physics
Volumen2025
N.º3
DOI
EstadoPublicada - mar 2025

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