Partial wave analysis of ψ3686→ΛΣ¯0π0 + c.c.

BESIII Collaboration

doi:10.1007/JHEP02(2025)212

Partial wave analysis of ψ3686→ΛΣ¯0π0 + c.c.

BESIII Collaboration

Instituto de Alta Investigación

CAS - Institute of High Energy Physics
Budker Institute of Nuclear Physics of the Siberian Branch of the RAS
Novosibirsk State University
Uppsala University
Ruhr University Bochum
Chinese Academy of Sciences
Zhengzhou University
Johannes Gutenberg University Mainz
University of Turin
National Institute for Nuclear Physics
University of Science and Technology of China
Southeast University, Nanjing
Joint Institute for Nuclear Research
Peking University
University of Chinese Academy of Sciences
National Centre for Nuclear Research
Mongolian Academy of Sciences
Carnegie Mellon University
University of Münster
Wuhan University
Istinye University
Nankai University
Moscow Institute of Physics and Technology
China University of Geosciences, Wuhan
Soochow University
Henan University
Nanjing University
North China Electric Power University
Tsinghua University
CAS - Institute of Modern Physics
Jilin University
Hunan University
Chung-Ang University
Shandong University
Yunnan University
Helmholtz Institute Mainz
University of South China
University of Jinan
Liaoning University
Sun Yat-Sen University
University of Eastern Piedmont
Nanjing Normal University
University of Ferrara
Henan Normal University
University of Manchester
University of Oxford
GSI Helmholtz Centre for Heavy Ion Research
Guangxi University
Shandong Normal University
Fudan University
Indiana University Bloomington
University of Hawai'i at Mānoa
Suranaree University of Technology
South China Normal University
University of the Punjab
Liaoning Normal University
Hangzhou Normal University
Huangshan College
University of Groningen
Indian Institute of Technology Madras
Justus Liebig University Giessen
Qufu Normal University
Renmin University of China
Lanzhou University
Hebei University
Sichuan University
Guangxi Normal University
Shanxi University
Central China Normal University
Henan University of Science and Technology
Henan University of Technology
Central South University
Zhejiang University
Goethe University Frankfurt
COMSATS University Islamabad
IBA
University of Perugia
Universidad de Tarapacá
Petersburg Nuclear Physics Institute (PNPI)
Hunan Normal University
China Center of Advanced Science and Technology World Laboratory
Swiss Federal Institute of Technology Lausanne
Shanghai Jiao Tong University
Ministry of Education of the People's Republic of China
Near East University
Beihang University
Inner Mongolia University
Yantai University
University of Bristol
Shanxi Normal University
University of Science and Technology Liaoning

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5 Citas (Scopus)

Resumen

Based on a sample of (2712.4 ± 14.3) × 10⁶ψ(3686) events collected with the BESIII detector, a partial wave analysis of the decay ψ3686→ΛΣ¯0π0 + c.c. is performed to investigate Λ^* and Σ^* resonances in the π0Σ¯0 and π⁰Λ invariant mass distributions. Significant contributions are found from the Λ(1405), Λ(1520), Λ(1600), Λ(1670), Λ(1690), Λ(1800), Λ(1890), Λ(2325), Σ(1385), Σ(1660), Σ(1670), Σ(1750), and Σ(1910). The masses, widths, and production branching fractions for each component are determined. In addition, the branching fraction of ψ3686→ΛΣ¯0π0 + c.c. is measured to be (1.544 ± 0.013 ± 0.071) × 10⁻⁴ for the first time, where the first uncertainty is statistical and the second systematic.

Idioma original	Inglés
Número de artículo	212
Publicación	Journal of High Energy Physics
Volumen	2025
N.º	2
DOI	https://doi.org/10.1007/JHEP02(2025)212
Estado	Publicada - feb 2025

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@article{5920c26283944d72b1040a7e1ccb0bff,

title = "Partial wave analysis of ψ3686→ΛΣ¯0π0 + c.c.",

abstract = "Based on a sample of (2712.4 ± 14.3) × 106ψ(3686) events collected with the BESIII detector, a partial wave analysis of the decay ψ3686→ΛΣ¯0π0 + c.c. is performed to investigate Λ* and Σ* resonances in the π0Σ¯0 and π0Λ invariant mass distributions. Significant contributions are found from the Λ(1405), Λ(1520), Λ(1600), Λ(1670), Λ(1690), Λ(1800), Λ(1890), Λ(2325), Σ(1385), Σ(1660), Σ(1670), Σ(1750), and Σ(1910). The masses, widths, and production branching fractions for each component are determined. In addition, the branching fraction of ψ3686→ΛΣ¯0π0 + c.c. is measured to be (1.544 ± 0.013 ± 0.071) × 10−4 for the first time, where the first uncertainty is statistical and the second systematic.",

keywords = "Branching fraction, Particle and Resonance Production, QCD, e-e Experiments",

author = "M. Ablikim and Achasov, \{M. N.\} and P. Adlarson and O. Afedulidis and S. Kabana and \{The BESIII collaboration\}",

note = "Publisher Copyright: {\textcopyright} The Author(s) 2025.",

year = "2025",

month = feb,

doi = "10.1007/JHEP02(2025)212",

language = "English",

volume = "2025",

journal = "Journal of High Energy Physics",

issn = "1126-6708",

number = "2",

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TY - JOUR

T1 - Partial wave analysis of ψ3686→ΛΣ¯0π0 + c.c.

AU - Ablikim, M.

AU - Achasov, M. N.

AU - Adlarson, P.

AU - Afedulidis, O.

AU - Kabana, S.

AU - The BESIII collaboration

N1 - Publisher Copyright: © The Author(s) 2025.

PY - 2025/2

Y1 - 2025/2

N2 - Based on a sample of (2712.4 ± 14.3) × 106ψ(3686) events collected with the BESIII detector, a partial wave analysis of the decay ψ3686→ΛΣ¯0π0 + c.c. is performed to investigate Λ* and Σ* resonances in the π0Σ¯0 and π0Λ invariant mass distributions. Significant contributions are found from the Λ(1405), Λ(1520), Λ(1600), Λ(1670), Λ(1690), Λ(1800), Λ(1890), Λ(2325), Σ(1385), Σ(1660), Σ(1670), Σ(1750), and Σ(1910). The masses, widths, and production branching fractions for each component are determined. In addition, the branching fraction of ψ3686→ΛΣ¯0π0 + c.c. is measured to be (1.544 ± 0.013 ± 0.071) × 10−4 for the first time, where the first uncertainty is statistical and the second systematic.

AB - Based on a sample of (2712.4 ± 14.3) × 106ψ(3686) events collected with the BESIII detector, a partial wave analysis of the decay ψ3686→ΛΣ¯0π0 + c.c. is performed to investigate Λ* and Σ* resonances in the π0Σ¯0 and π0Λ invariant mass distributions. Significant contributions are found from the Λ(1405), Λ(1520), Λ(1600), Λ(1670), Λ(1690), Λ(1800), Λ(1890), Λ(2325), Σ(1385), Σ(1660), Σ(1670), Σ(1750), and Σ(1910). The masses, widths, and production branching fractions for each component are determined. In addition, the branching fraction of ψ3686→ΛΣ¯0π0 + c.c. is measured to be (1.544 ± 0.013 ± 0.071) × 10−4 for the first time, where the first uncertainty is statistical and the second systematic.

KW - Branching fraction

KW - Particle and Resonance Production

KW - QCD

KW - e-e Experiments

UR - https://www.scopus.com/pages/publications/105018587827

U2 - 10.1007/JHEP02(2025)212

DO - 10.1007/JHEP02(2025)212

M3 - Article

AN - SCOPUS:105018587827

SN - 1126-6708

VL - 2025

JO - Journal of High Energy Physics

JF - Journal of High Energy Physics

IS - 2

M1 - 212

ER -

Partial wave analysis of ψ3686→ΛΣ¯0π0 + c.c.

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