TY - JOUR
T1 - Measurement of the Time-Integrated πΆβ’π Asymmetry in π·0βπΎββ’πΎ+ Decays
AU - LHCb collaboration
AU - Barter, William
AU - Clarke, P.E.L.
AU - Gambetta, S.
AU - Muheim, F.
AU - Needham, M.
AU - Williams, Mark
AU - Betti, Federico
AU - Currie, Robert
AU - Eisenhardt, S.
AU - Lavra, Lais Soares
AU - Federica, Oliva
AU - Ozcelik, Ozlem
AU - Sarpis, Gediminas
AU - O'Neil, R.H.
AU - Richardson-Slipper, M.
AU - Vrahas, C.
PY - 2023/8/29
Y1 - 2023/8/29
N2 - The time-integrated πΆβ’π asymmetry in the Cabibbo-suppressed decay π·0βπΎββ’πΎ+ is measured using proton-proton collision data, corresponding to an integrated luminosity of 5.7ββfbβ1 collected at a center-of-mass energy of 13 TeV with the LHCb detector. The π·0 mesons are required to originate from promptly produced π·*+βπ·0β’π+ decays, and the charge of the companion pion is used to determine the flavor of the charm meson at production. The time-integrated πΆβ’π asymmetry is measured to be ππΆβ’πβ‘(πΎββ’πΎ+)=[6.8Β±5.4Β±1.6]Γ10β4 where the first uncertainty is statistical and the second systematic. The direct πΆβ’π asymmetries in π·0βπΎββ’πΎ+ and π·0βπββ’π+ decays, πππΎββ’πΎ+ and πππββ’π+, are derived by combining ππΆβ’πβ‘(πΎββ’πΎ+) with the time-integrated πΆβ’π asymmetry difference, Ξβ’π΄πΆβ’π=ππΆβ’πβ‘(πΎββ’πΎ+)βππΆβ’πβ‘(πββ’π+), and other inputs, giving πππΎββ’πΎ+=(7.7Β±5.7)Γ10β4,πππββ’π+=(23.2Β±6.1)Γ10β4,with a correlation coefficient corresponding to π=0.88. The compatibility of these results with πΆβ’π symmetry is 1.4 and 3.8 standard deviations for π·0βπΎββ’πΎ+ and π·0βπββ’π+ decays, respectively. This is the first evidence for direct πΆβ’π violation in a specific π·0 decay.
AB - The time-integrated πΆβ’π asymmetry in the Cabibbo-suppressed decay π·0βπΎββ’πΎ+ is measured using proton-proton collision data, corresponding to an integrated luminosity of 5.7ββfbβ1 collected at a center-of-mass energy of 13 TeV with the LHCb detector. The π·0 mesons are required to originate from promptly produced π·*+βπ·0β’π+ decays, and the charge of the companion pion is used to determine the flavor of the charm meson at production. The time-integrated πΆβ’π asymmetry is measured to be ππΆβ’πβ‘(πΎββ’πΎ+)=[6.8Β±5.4Β±1.6]Γ10β4 where the first uncertainty is statistical and the second systematic. The direct πΆβ’π asymmetries in π·0βπΎββ’πΎ+ and π·0βπββ’π+ decays, πππΎββ’πΎ+ and πππββ’π+, are derived by combining ππΆβ’πβ‘(πΎββ’πΎ+) with the time-integrated πΆβ’π asymmetry difference, Ξβ’π΄πΆβ’π=ππΆβ’πβ‘(πΎββ’πΎ+)βππΆβ’πβ‘(πββ’π+), and other inputs, giving πππΎββ’πΎ+=(7.7Β±5.7)Γ10β4,πππββ’π+=(23.2Β±6.1)Γ10β4,with a correlation coefficient corresponding to π=0.88. The compatibility of these results with πΆβ’π symmetry is 1.4 and 3.8 standard deviations for π·0βπΎββ’πΎ+ and π·0βπββ’π+ decays, respectively. This is the first evidence for direct πΆβ’π violation in a specific π·0 decay.
U2 - 10.1103/PhysRevLett.131.091802
DO - 10.1103/PhysRevLett.131.091802
M3 - Article
SN - 0031-9007
VL - 131
SP - 1
EP - 13
JO - Physical Review Letters
JF - Physical Review Letters
IS - 9
M1 - 091802
ER -