TY - JOUR
T1 - First Measurement of the Decay Dynamics in the Semileptonic Transition of D+ (0) into the Axial-Vector Meson K ¯ 1 (1270)
AU - Ablikim, M.
AU - Achasov, M. N.
AU - Adlarson, P.
AU - Ai, X. C.
AU - Kabana, S.
AU - The BESIII collaboration
N1 - Publisher Copyright:
© 2025 authors. Published by the American Physical Society.
PY - 2025/8/29
Y1 - 2025/8/29
N2 - Using e+e- data taken at the center-of-mass energy of 3.773 GeV with the BESIII detector, corresponding to an integrated luminosity of 20.3 fb-1, we report the first measurement of the decay dynamics of the semileptonic decays D+(0)→K-π+π0(-)e+νe. The amplitude analysis gives the hadronic form factors of the semileptonic D transitions into the axial-vector meson K̄1(1270) to be rA=(-11.2±1.0stat±0.9syst)×10-2 and rV=(-4.3±1.0stat±2.5syst)×10-2. This is the first in the semileptonic decays of heavy mesons into axial-vector mesons. The angular analysis yields an up-down asymmetry Aud′=0.01±0.11, which is consistent with the standard model prediction. In addition, the branching fractions of D+→K̄1(1270)0e+νe and D0→K1(1270)-e+νe are determined with improved precision to be (2.27±0.11stat±0.07syst±0.07input)×10-3 and (1.02±0.06stat±0.06syst±0.03input)×10-3, respectively. No significant signals of D+→K̄1(1400)0e+νe and D0→K1(1400)-e+νe are observed and their branching fraction upper limits are set as 1.4×10-4 and 0.7×10-4 at 90% confidence level, respectively.
AB - Using e+e- data taken at the center-of-mass energy of 3.773 GeV with the BESIII detector, corresponding to an integrated luminosity of 20.3 fb-1, we report the first measurement of the decay dynamics of the semileptonic decays D+(0)→K-π+π0(-)e+νe. The amplitude analysis gives the hadronic form factors of the semileptonic D transitions into the axial-vector meson K̄1(1270) to be rA=(-11.2±1.0stat±0.9syst)×10-2 and rV=(-4.3±1.0stat±2.5syst)×10-2. This is the first in the semileptonic decays of heavy mesons into axial-vector mesons. The angular analysis yields an up-down asymmetry Aud′=0.01±0.11, which is consistent with the standard model prediction. In addition, the branching fractions of D+→K̄1(1270)0e+νe and D0→K1(1270)-e+νe are determined with improved precision to be (2.27±0.11stat±0.07syst±0.07input)×10-3 and (1.02±0.06stat±0.06syst±0.03input)×10-3, respectively. No significant signals of D+→K̄1(1400)0e+νe and D0→K1(1400)-e+νe are observed and their branching fraction upper limits are set as 1.4×10-4 and 0.7×10-4 at 90% confidence level, respectively.
UR - https://www.scopus.com/pages/publications/105016055819
U2 - 10.1103/xj42-xgzf
DO - 10.1103/xj42-xgzf
M3 - Article
C2 - 40952235
AN - SCOPUS:105016055819
SN - 0031-9007
VL - 135
JO - Physical Review Letters
JF - Physical Review Letters
IS - 9
M1 - 091801
ER -