Research output: Contribution to journal › Article › peer-review
Partial wave analysis of the charmed baryon hadronic decay Λc+ → Λπ + π 0. / Ачасов, Михаил Николаевич; Мучной, Николай Юрьевич; Николаев, Иван Борисович.
In: Journal of High Energy Physics, 06.12.2022.Research output: Contribution to journal › Article › peer-review
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TY - JOUR
T1 - Partial wave analysis of the charmed baryon hadronic decay Λc+ → Λπ + π 0
AU - Ачасов, Михаил Николаевич
AU - Мучной, Николай Юрьевич
AU - Николаев, Иван Борисович
N1 - Публикация для проверки.
PY - 2022/12/6
Y1 - 2022/12/6
N2 - Based on e+e− collision samples corresponding to an integrated luminosity of 4.4 fb−1 collected with the BESIII detector at center-of-mass energies between 4.6 GeV and 4.7 GeV, a partial wave analysis of the charmed baryon hadronic decay Λ+c → Λπ+π0 is performed, and the decays Λ+c → Λρ(770)+ and Λ+c → Σ(1385)π are studied for the first time. Making use of the world-average branching fraction B(Λ+c→Λπ+π0), their branching fractions are determined to be B(Λ+c→Λρ(770)+)=(4.06±0.30±0.35±0.23)×10−2,B(Λ+c→Σ(1385)+π0)=(5.86±0.49±0.52±0.35)×10−3,B(Λ+c→Σ(1385)0π+)=(6.47±0.59±0.66±0.38)×10−3, where the first uncertainties are statistical, the second are systematic, and the third are from the uncertainties of the branching fractions B(Λ+c→Λπ+π0) and B(Σ(1385)→Λπ). In addition, the decay asymmetry parameters are measured to be αΛρ(770)+ = − 0.763 ± 0.053 ± 0.045, αΣ(1385)+π0=−0.917±0.069±0.056, and αΣ(1385)0π+=−0.789±0.098±0.056.
AB - Based on e+e− collision samples corresponding to an integrated luminosity of 4.4 fb−1 collected with the BESIII detector at center-of-mass energies between 4.6 GeV and 4.7 GeV, a partial wave analysis of the charmed baryon hadronic decay Λ+c → Λπ+π0 is performed, and the decays Λ+c → Λρ(770)+ and Λ+c → Σ(1385)π are studied for the first time. Making use of the world-average branching fraction B(Λ+c→Λπ+π0), their branching fractions are determined to be B(Λ+c→Λρ(770)+)=(4.06±0.30±0.35±0.23)×10−2,B(Λ+c→Σ(1385)+π0)=(5.86±0.49±0.52±0.35)×10−3,B(Λ+c→Σ(1385)0π+)=(6.47±0.59±0.66±0.38)×10−3, where the first uncertainties are statistical, the second are systematic, and the third are from the uncertainties of the branching fractions B(Λ+c→Λπ+π0) and B(Σ(1385)→Λπ). In addition, the decay asymmetry parameters are measured to be αΛρ(770)+ = − 0.763 ± 0.053 ± 0.045, αΣ(1385)+π0=−0.917±0.069±0.056, and αΣ(1385)0π+=−0.789±0.098±0.056.
U2 - 10.1007/JHEP12(2022)033
DO - 10.1007/JHEP12(2022)033
M3 - Article
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
SN - 1029-8479
M1 - 33
ER -
ID: 55696691