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.

First Measurement of the Decay Dynamics in the Semileptonic Transition of D+(0) into the Axial-Vector Meson K¯1(1270)

Amoroso, A.;Bianchi, F.;Bortone, A.;Destefanis, M.;De Mori, F.;Greco, M.;Maggiora, M.;Marcello, S.;Sosio, S.;Spataro, S.;
2025-01-01

Abstract

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.
2025
135
9
1
12
Ablikim, M.; Achasov, M. N.; Adlarson, P.; Ai, X. C.; Aliberti, R.; Amoroso, A.; An, Q.; Bai, Y.; Bakina, O.; Ban, Y.; Bao, H.-R.; Batozskaya, V.; Beg...espandi
File in questo prodotto:
File Dimensione Formato  
xj42-xgzf.pdf

Accesso aperto

Tipo di file: PDF EDITORIALE
Dimensione 1.03 MB
Formato Adobe PDF
1.03 MB Adobe PDF Visualizza/Apri

I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/2117669
Citazioni
  • ???jsp.display-item.citation.pmc??? 1
  • Scopus 1
  • ???jsp.display-item.citation.isi??? 0
social impact