Measurement of the branching fraction of DDs+ ? ?+?? via ?+ ? ?+????
dc.authorid | Tian, Zhifu/0000-0002-6592-9844 | |
dc.authorid | Huang, Kexin/0000-0001-6693-8390 | |
dc.authorid | Liu, Donghua/0000-0002-5830-9540 | |
dc.authorid | Li, Yuanyuan/0000-0002-4955-1159 | |
dc.authorid | Qin, Jiajun/0000-0002-9956-2358 | |
dc.authorid | Farineli, Riccardo/0000-0002-7972-9093 | |
dc.authorid | Wei, Wei/0000-0002-4109-3878 | |
dc.authorwosid | Yuan, Fang/JQV-7426-2023 | |
dc.authorwosid | Huang, Yong/KFA-1191-2024 | |
dc.authorwosid | GAO, Yang/HMO-8142-2023 | |
dc.authorwosid | lu, kai/KBB-4008-2024 | |
dc.authorwosid | zhang, quan/KHY-9180-2024 | |
dc.authorwosid | Zhang, Han/JMR-0670-2023 | |
dc.authorwosid | Tian, Zhifu/ABD-8799-2021 | |
dc.contributor.author | Ablikim, M. | |
dc.contributor.author | Achasov, M. N. | |
dc.contributor.author | Adlarson, P. | |
dc.contributor.author | Ai, X. C. | |
dc.contributor.author | Aliberti, R. | |
dc.contributor.author | Amoroso, A. | |
dc.contributor.author | Çetin, Serkant Ali | |
dc.date.accessioned | 2024-05-19T14:41:01Z | |
dc.date.available | 2024-05-19T14:41:01Z | |
dc.date.issued | 2023 | |
dc.department | İstinye Üniversitesi | en_US |
dc.description.abstract | Utilizing 7.33 fb(-1) of e(+)e(-) collision data taken at the center-of-mass energies of 4.128, 4.157, 4.178, 4.189, 4.199, 4.209, 4.219, and 4.226 GeV with the BESIII detector, the branching fraction of the leptonic decay D+s+ -> tau(+)nu(tau) via tau(+) -> mu(+)nu(mu )is measured to be BD+s ->tau+nu tau = (5.37 +/- 0.17(stat) +/- 0.15(syst))%. Combining this branching fraction with the world averages of the measurements of the masses of tau(+) and D-s(+) as well as the lifetime of D-s(+) , we extract the product of the decay constant of D-s(+) and the c -> s Cabibbo-Kobayashi-Maskawa matrix element to be D- f(s)+ |V-cs| = (246.7 +/- 3.9(stat) +/- 3.6(syst)) MeV. Taking |V-cs| from a global fit in the standard model we obtain fD+s = (253.4 +/- 4.0(stat) +/- 3.7(syst)) MeV. Conversely, taking( f)D(s)(+) from lattice quantum chromodynamics calculations, we obtain |V-cs| = 0.987 +/- 0.016(stat) +/- 0.014(syst). | en_US |
dc.description.sponsorship | The BESIII collaboration thanks the staff of BEPCII and the IHEP computing center for their strong support. This work is supported in part by National Key Ramp;D Program of China under Contracts Nos. 2020YFA0406400, 2020YFA0406300; National Natural Scienc; IHEP computing center [2020YFA0406400, 2020YFA0406300]; National Key Ramp;D Program of China [11875170, 12105076, 11635010, 11735014, 11835012, 11935015, 11935016, 11935018, 11961141012, 12022510, 12025502, 12035009, 12035013, 12061131003, 12192260, 12192261, 12192262, 12192263, 12192264, 12192265]; National Natural Science Foundation of China (NSFC); Chinese Academy of Sciences (CAS) Large-Scale Scientific Facility Program; CAS Center for Excellence in Particle Physics (CCEPP); Joint Large-Scale Scientific Facility Funds of the NSFC [U1832207]; CAS [QYZDJ-SSW-SLH003, QYZDJ-SSW-SLH040]; CAS Key Research Program of Frontier Sciences; 100 Talents Program of CAS; Institute of Nuclear and Particle Physics (INPAC); Shanghai Key Laboratory for Particle Physics and Cosmology [758462]; ERC [894790]; European Union [443159800, 455635585, CRC 1044, FOR5327, GRK 2149]; German Research Foundation DFG; Istituto Nazionale di Fisica Nucleare, Italy [DPT2006K-120470]; Ministry of Development of Turkey [NRF-2022R1A2C1092335]; National Research Foundation of Korea; National Science and Technology fund [B16F640076]; National Science Research and Innovation Fund (NSRF) via the Program Management Unit for Human Resources amp; Institutional Development, Research and Innovation [2019/35/O/ST2/02907]; Polish National Science Centre; Suranaree University of Technology (SUT), Thailand Science Research and Innovation (TSRI) [160355]; National Science Research and Innovation Fund (NSRF) [DH160214]; Royal Society, U.K.; Swedish Research Council [DE-FG02-05ER41374]; U.S. Department of Energy | en_US |
dc.description.sponsorship | The BESIII collaboration thanks the staff of BEPCII and the IHEP computing center for their strong support. This work is supported in part by National Key R&D Program of China under Contracts Nos. 2020YFA0406400, 2020YFA0406300; National Natural Science Foundation of China (NSFC) under Contracts Nos. 11875170, 12105076, 11635010, 11735014, 11835012, 11935015, 11935016, 11935018, 11961141012, 12022510, 12025502, 12035009, 12035013, 12061131003, 12192260, 12192261, 12192262, 12192263, 12192264, 12192265; the Chinese Academy of Sciences (CAS) Large-Scale Scientific Facility Program; the CAS Center for Excellence in Particle Physics (CCEPP); Joint Large-Scale Scientific Facility Funds of the NSFC and CAS under Contract No. U1832207; CAS Key Research Program of Frontier Sciences under Contracts Nos. QYZDJ-SSW-SLH003, QYZDJ-SSW-SLH040; 100 Talents Program of CAS; The Institute of Nuclear and Particle Physics (INPAC) and Shanghai Key Laboratory for Particle Physics and Cosmology; ERC under Contract No. 758462; European Union's Horizon 2020 research and innovation programme under Marie Sklodowska-Curie grant agreement under Contract No. 894790; German Research Foundation DFG under Contracts Nos. 443159800, 455635585, Collaborative Research Center CRC 1044, FOR5327, GRK 2149; Istituto Nazionale di Fisica Nucleare, Italy; Ministry of Development of Turkey under Contract No. DPT2006K-120470; National Research Foundation of Korea under Contract No. NRF-2022R1A2C1092335; National Science and Technology fund; National Science Research and Innovation Fund (NSRF) via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation under Contract No. B16F640076; Polish National Science Centre under Contract No. 2019/35/O/ST2/02907; Suranaree University of Technology (SUT), Thailand Science Research and Innovation (TSRI), and National Science Research and Innovation Fund (NSRF) under Contract No. 160355; The Royal Society, U.K. under Contract No. DH160214; The Swedish Research Council; U.S. Department of Energy under Contract No. DE-FG02-05ER41374. | en_US |
dc.identifier.doi | 10.1007/JHEP09(2023)124 | |
dc.identifier.issn | 1029-8479 | |
dc.identifier.issue | 9 | en_US |
dc.identifier.scopus | 2-s2.0-85171844530 | en_US |
dc.identifier.scopusquality | Q2 | en_US |
dc.identifier.uri | https://doi.org10.1007/JHEP09(2023)124 | |
dc.identifier.uri | https://hdl.handle.net/20.500.12713/5051 | |
dc.identifier.wos | WOS:001095457100001 | en_US |
dc.identifier.wosquality | N/A | en_US |
dc.indekslendigikaynak | Web of Science | en_US |
dc.indekslendigikaynak | Scopus | en_US |
dc.language.iso | en | en_US |
dc.publisher | Springer | en_US |
dc.relation.ispartof | Journal of High Energy Physics | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.rights | info:eu-repo/semantics/openAccess | en_US |
dc.snmz | 20240519_ka | en_US |
dc.subject | E(+)-E(-) Experiments | en_US |
dc.title | Measurement of the branching fraction of DDs+ ? ?+?? via ?+ ? ?+???? | en_US |
dc.type | Article | en_US |