Standard

Measurement of the branching fractions of χcJ→ π+π−π0π0 via ψ(3686) → γχcJ. / The BESIII Collaboration ; Ачасов, Михаил Николаевич; Мучной, Николай Юрьевич и др.

в: Journal of High Energy Physics, Том 2026, № 8, 23, 05.08.2026.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

Harvard

APA

Vancouver

The BESIII Collaboration, Ачасов МН, Мучной НЮ, Николаев ИБ. Measurement of the branching fractions of χcJ→ π+π−π0π0 via ψ(3686) → γχcJ. Journal of High Energy Physics. 2026 авг. 5;2026(8):23. doi: 10.1007/JHEP08(2026)023

Author

BibTeX

@article{41530c6eec7c47a4b8530cc6d325623c,
title = "Measurement of the branching fractions of χcJ→ π+π−π0π0 via ψ(3686) → γχcJ",
abstract = "Using (2712.4 ± 14.3) × 106 ψ(3686) events collected with the BESIII detector operating at BEPCII, the branching fractions of χcJ → π+π−π0π0 (J = 0, 1, 2) are measured via the radiative transition ψ(3686) → γχcJ. The results are ℬ(χc0 → π+π−π0π0) = (3.10 ± 0.01 ± 0.14) × 10−2, ℬ(χc1 → π+π−π0π0) = (1.16 ± 0.01 ± 0.05) × 10−2, and B(χc2 → π+π−π0π0) = (1.92 ± 0.01 ± 0.08) × 10−2, where the first uncertainties are statistical and the second systematic. The dominant intermediate states are found to be χcJ → ρ+ρ−. These results improve upon previous measurements with significantly enhanced precision.",
keywords = "Branching fraction, Charm Physics, e +-e − Experiments",
author = "{BESIII Collaboration} and Ачасов, {Михаил Николаевич} and Мучной, {Николай Юрьевич} and Николаев, {Иван Борисович}",
note = "The BESIII Collaboration thanks the staff of BEPCII (https://cstr.cn/31109.02.BEPC) and the IHEP computing center for their strong support. This work is supported in part by National Key R&D Program of China under Contracts Nos. 2025YFA1613900, 2023YFA1606000, 2023YFA1606704; National Natural Science Foundation of China (NSFC) under Contracts Nos. 11635010, 11935015, 11935016, 11935018, 12025502, 12035009, 12035013, 12061131003, 12192260, 12192261, 12192262, 12192263, 12192264, 12192265, 12221005, 12225509, 12235017, 12342502, 12361141819; the Chinese Academy of Sciences (CAS) Large-Scale Scientific Facility Program; the Strategic Priority Research Program of Chinese Academy of Sciences under Contract No. XDA0480600; CAS under Contract No. YSBR-101; 100 Talents Program of CAS; The Institute of Nuclear and Particle Physics (INPAC) and Shanghai Key Laboratory for Particle Physics and Cosmology; ERC under Contract No. 758462; German Research Foundation DFG under Contract No. FOR5327; Istituto Nazionale di Fisica Nucleare, Italy; Knut and Alice Wallenberg Foundation under Contracts Nos. 2021.0174, 2021.0299, 2023.0315; Ministry of Development of Turkey under Contract No. DPT2006K-120470; National Research Foundation of Korea under Contract No. NRF-2022R1A2C1092335; National Science and Technology fund of Mongolia; Polish National Science Centre under Contract No. 2024/53/B/ST2/00975; STFC (United Kingdom); Swedish Research Council under Contract No. 2019.04595; U.S. Department of Energy under Contract No. DE-FG02-05ER41374.",
year = "2026",
month = aug,
day = "5",
doi = "10.1007/JHEP08(2026)023",
language = "English",
volume = "2026",
journal = "Journal of High Energy Physics",
issn = "1029-8479",
publisher = "Springer US",
number = "8",

}

RIS

TY - JOUR

T1 - Measurement of the branching fractions of χcJ→ π+π−π0π0 via ψ(3686) → γχcJ

AU - BESIII Collaboration

AU - Ачасов, Михаил Николаевич

AU - Мучной, Николай Юрьевич

AU - Николаев, Иван Борисович

N1 - The BESIII Collaboration thanks the staff of BEPCII (https://cstr.cn/31109.02.BEPC) and the IHEP computing center for their strong support. This work is supported in part by National Key R&D Program of China under Contracts Nos. 2025YFA1613900, 2023YFA1606000, 2023YFA1606704; National Natural Science Foundation of China (NSFC) under Contracts Nos. 11635010, 11935015, 11935016, 11935018, 12025502, 12035009, 12035013, 12061131003, 12192260, 12192261, 12192262, 12192263, 12192264, 12192265, 12221005, 12225509, 12235017, 12342502, 12361141819; the Chinese Academy of Sciences (CAS) Large-Scale Scientific Facility Program; the Strategic Priority Research Program of Chinese Academy of Sciences under Contract No. XDA0480600; CAS under Contract No. YSBR-101; 100 Talents Program of CAS; The Institute of Nuclear and Particle Physics (INPAC) and Shanghai Key Laboratory for Particle Physics and Cosmology; ERC under Contract No. 758462; German Research Foundation DFG under Contract No. FOR5327; Istituto Nazionale di Fisica Nucleare, Italy; Knut and Alice Wallenberg Foundation under Contracts Nos. 2021.0174, 2021.0299, 2023.0315; Ministry of Development of Turkey under Contract No. DPT2006K-120470; National Research Foundation of Korea under Contract No. NRF-2022R1A2C1092335; National Science and Technology fund of Mongolia; Polish National Science Centre under Contract No. 2024/53/B/ST2/00975; STFC (United Kingdom); Swedish Research Council under Contract No. 2019.04595; U.S. Department of Energy under Contract No. DE-FG02-05ER41374.

PY - 2026/8/5

Y1 - 2026/8/5

N2 - Using (2712.4 ± 14.3) × 106 ψ(3686) events collected with the BESIII detector operating at BEPCII, the branching fractions of χcJ → π+π−π0π0 (J = 0, 1, 2) are measured via the radiative transition ψ(3686) → γχcJ. The results are ℬ(χc0 → π+π−π0π0) = (3.10 ± 0.01 ± 0.14) × 10−2, ℬ(χc1 → π+π−π0π0) = (1.16 ± 0.01 ± 0.05) × 10−2, and B(χc2 → π+π−π0π0) = (1.92 ± 0.01 ± 0.08) × 10−2, where the first uncertainties are statistical and the second systematic. The dominant intermediate states are found to be χcJ → ρ+ρ−. These results improve upon previous measurements with significantly enhanced precision.

AB - Using (2712.4 ± 14.3) × 106 ψ(3686) events collected with the BESIII detector operating at BEPCII, the branching fractions of χcJ → π+π−π0π0 (J = 0, 1, 2) are measured via the radiative transition ψ(3686) → γχcJ. The results are ℬ(χc0 → π+π−π0π0) = (3.10 ± 0.01 ± 0.14) × 10−2, ℬ(χc1 → π+π−π0π0) = (1.16 ± 0.01 ± 0.05) × 10−2, and B(χc2 → π+π−π0π0) = (1.92 ± 0.01 ± 0.08) × 10−2, where the first uncertainties are statistical and the second systematic. The dominant intermediate states are found to be χcJ → ρ+ρ−. These results improve upon previous measurements with significantly enhanced precision.

KW - Branching fraction

KW - Charm Physics

KW - e +-e − Experiments

UR - https://www.scopus.com/pages/publications/105049210618

U2 - 10.1007/JHEP08(2026)023

DO - 10.1007/JHEP08(2026)023

M3 - Article

VL - 2026

JO - Journal of High Energy Physics

JF - Journal of High Energy Physics

SN - 1029-8479

IS - 8

M1 - 23

ER -

ID: 83280689