Using collision data corresponding to an integrated luminosity of recorded by the BESIII detector at center-of-mass energies between 4.128 and 4.226 GeV, we present an analysis of the decay , where the is produced via the process . We observe the in the system and the branching fraction of the decay with measured to be , where the uncertainties are statistical and systematic, respectively. The dynamics of the decay are studied with the simple pole parametrization of the hadronic form factor and the Flatté formula describing the in the differential decay rate, and the product of the form factor and the Cabibbo-Kobayashi-Maskawa matrix element is determined for the first time to be . Furthermore, the decay is searched for the first time but no signal is found. The upper limit on the branching fraction of , decay is set to be at 90% confidence level.
@article{osti_2335437,
author = {Ablikim, M. and Achasov, M. N. and Adlarson, P. and Aliberti, R. and Amoroso, A. and An, M. R. and An, Q. and Bai, Y. and Bakina, O. and Balossino, I. and others},
title = {Study of the <math display='inline'> <msub> <mi>f</mi> <mn>0</mn> </msub> <mo stretchy='false'>(</mo> <mn>980</mn> <mo stretchy='false'>)</mo> </math> and <math display='inline'> <mrow> <msub> <mrow> <mi>f</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> <mo stretchy='false'>(</mo> <mn>500</mn> <mo stretchy='false'>)</mo> </mrow> </math> Scalar Mesons through the Decay <math display='inline'> <mrow> <msubsup> <mrow> <mi>D</mi> </mrow> <mrow> <mi>s</mi> </mrow> <mrow> <mo>+</mo> </mrow> </msubsup> <mo stretchy='false'>→</mo> <msup> <mrow> <mi>π</mi> </mrow> <mrow> <mo>+</mo> </mrow> </msup> <msup> <mrow> <mi>π</mi> </mrow> <mrow> <mo>−</mo> </mrow> </msup> <msup> <mrow> <mi>e</mi> </mrow> <mrow> <mo>+</mo> </mrow> </msup> <msub> <mrow> <mi>ν</mi> </mrow> <mrow> <mi>e</mi> </mrow> </msub> </mrow> </math>},
annote = { Using e + e − collision data corresponding to an integrated luminosity of 7.33 fb − 1 recorded by the BESIII detector at center-of-mass energies between 4.128 and 4.226 GeV, we present an analysis of the decay D s + → π + π − e + ν e , where the D s + is produced via the process e + e − → D s * ± D s ∓ . We observe the f 0 ( 980 ) in the π + π − system and the branching fraction of the decay D s + → f 0 ( 980 ) e + ν e with f 0 ( 980 ) → π + π − measured to be ( 1.72 ± 0.1 3 stat ± 0.1 0 syst ) × 10 − 3 , where the uncertainties are statistical and systematic, respectively. The dynamics of the D s + → f 0 ( 980 ) e + ν e decay are studied with the simple pole parametrization of the hadronic form factor and the Flatté formula describing the f 0 ( 980 ) in the differential decay rate, and the product of the form factor f + f 0 ( 0 ) and the c → s Cabibbo-Kobayashi-Maskawa matrix element | V c s | is determined for the first time to be f + f 0 ( 0 ) | V c s | = 0.504 ± 0.01 7 stat ± 0.03 5 syst . Furthermore, the decay D s + → f 0 ( 500 ) e + ν e is searched for the first time but no signal is found. The upper limit on the branching fraction of D s + → f 0 ( 500 ) e + ν e , f 0 ( 500 ) → π + π − decay is set to be 3.3 × 10 − 4 at 90% confidence level. Published by the American Physical Society 2024 },
doi = {10.1103/PhysRevLett.132.141901},
url = {https://www.osti.gov/biblio/2335437},
journal = {Physical Review Letters},
issn = {ISSN PRLTAO},
number = {14},
volume = {132},
place = {United States},
publisher = {American Physical Society},
year = {2024},
month = {04}}
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, Vol. 462, Issue 1-2https://doi.org/10.1016/S0168-9002(01)00089-4
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, Vol. 506, Issue 3https://doi.org/10.1016/S0168-9002(03)01368-8
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, Vol. 614, Issue 3https://doi.org/10.1016/j.nima.2009.12.050