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Amplitude analysis of the decays D0 → π+π−π+π− and D0 → π+π−π0π0*. / The BESIII Collaboration ; Мучной, Николай Юрьевич.

в: Chinese Physics C, Том 48, № 8, 083001, 01.08.2024.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

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The BESIII Collaboration, Мучной НЮ. Amplitude analysis of the decays D0 → π+π−π+π− and D0 → π+π−π0π0*. Chinese Physics C. 2024 авг. 1;48(8):083001. doi: 10.1088/1674-1137/ad3d4d

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@article{7310bbfd9af44d95b83e8f167b083337,
title = "Amplitude analysis of the decays D0 → π+π−π+π− and D0 → π+π−π0π0*",
abstract = "Using e+e− annihilation data corresponding to an integrated luminosity of 2.93 fb−1 taken at the center-of-mass energy √s = 3.773 GeV with the BESIII detector, a joint amplitude analysis is performed on the decays D0 → π+π−π+π− and D0 → π+π−π0π0 (non-η). The fit fractions of individual components are obtained, and large interferences among the dominant components of the decays D0 → a1(1260)π, D0 → π(1300)π, D0 → ρ(770)ρ(770), and D0 → 2(ππ)S are observed in both channels. With the obtained amplitude model, the CP-even fractions of D0 → π+π−π+π− and D0 → π+π−π0π0 (non-η) are determined to be (75.2 ± 1.1stat. ± 1.5syst.) % and (68.9 ± 1.5stat. ± 2.4syst.)%, respectively. The branching fractions of D0 → π+π−π+π− and D0 → π+π−π0π0 (non-η) are measured to be (0.688 ± 0.010stat. ± 0.010syst.)% and (0.951 ± 0.025stat. ± 0.021syst.)%, respectively. The amplitude analysis provides an important model for the binning strategy in measuring the strong phase parameters of D0 → 4π when used to determine the CKM angle γ(ϕ3) via the B− → DK− decay. ",
keywords = "BESIII, CP-even fraction, D0 meson decays, amplitude analysis",
author = "{BESIII Collaboration} and {Ablikim 麦}, {M. 迪娜} and Achasov, {M. n.} and P. Adlarson and O. Afedulidis and {Ai 艾}, {X. c. 小聪} and R. Aliberti and A. Amoroso and {An 安}, {Q. 琪} and {Bai 白}, {Y. 羽} and O. Bakina and I. Balossino and {Ban 班}, {Y. 勇} and {Bao 包}, {H.-R. 浩然} and V. Batozskaya and K. Begzsuren and N. Berger and M. Berlowski and M. Bertani and D. Bettoni and F. Bianchi and E. Bianco and A. Bortone and Briere, {R. a.} and A. Brueggemann and {Cai 蔡}, {H. 浩} and {Cai 蔡}, {X. 啸} and A. Calcaterra and {Cao 曹}, {G. f. 国富} and {Cao 曹}, {N. 宁} and Cetin, {S. a.} and {Chang 常}, {J. f. 劲帆} and Chang, {W. l.} and {Che 车}, {G. r. 国荣} and G. Chelkov and {Chen 陈}, {C. 琛} and {Chen 陈}, {C. h. 春卉} and {Chen 陈}, {Chao 超} and Nikolaev, {I. b.} and Мучной, {Николай Юрьевич}",
year = "2024",
month = aug,
day = "1",
doi = "10.1088/1674-1137/ad3d4d",
language = "English",
volume = "48",
journal = "Chinese Physics C",
issn = "1674-1137",
publisher = "IOP Publishing Ltd.",
number = "8",

}

RIS

TY - JOUR

T1 - Amplitude analysis of the decays D0 → π+π−π+π− and D0 → π+π−π0π0*

AU - BESIII Collaboration

AU - Ablikim 麦, M. 迪娜

AU - Achasov, M. n.

AU - Adlarson, P.

AU - Afedulidis, O.

AU - Ai 艾, X. c. 小聪

AU - Aliberti, R.

AU - Amoroso, A.

AU - An 安, Q. 琪

AU - Bai 白, Y. 羽

AU - Bakina, O.

AU - Balossino, I.

AU - Ban 班, Y. 勇

AU - Bao 包, H.-R. 浩然

AU - Batozskaya, V.

AU - Begzsuren, K.

AU - Berger, N.

AU - Berlowski, M.

AU - Bertani, M.

AU - Bettoni, D.

AU - Bianchi, F.

AU - Bianco, E.

AU - Bortone, A.

AU - Briere, R. a.

AU - Brueggemann, A.

AU - Cai 蔡, H. 浩

AU - Cai 蔡, X. 啸

AU - Calcaterra, A.

AU - Cao 曹, G. f. 国富

AU - Cao 曹, N. 宁

AU - Cetin, S. a.

AU - Chang 常, J. f. 劲帆

AU - Chang, W. l.

AU - Che 车, G. r. 国荣

AU - Chelkov, G.

AU - Chen 陈, C. 琛

AU - Chen 陈, C. h. 春卉

AU - Chen 陈, Chao 超

AU - Nikolaev, I. b.

AU - Мучной, Николай Юрьевич

PY - 2024/8/1

Y1 - 2024/8/1

N2 - Using e+e− annihilation data corresponding to an integrated luminosity of 2.93 fb−1 taken at the center-of-mass energy √s = 3.773 GeV with the BESIII detector, a joint amplitude analysis is performed on the decays D0 → π+π−π+π− and D0 → π+π−π0π0 (non-η). The fit fractions of individual components are obtained, and large interferences among the dominant components of the decays D0 → a1(1260)π, D0 → π(1300)π, D0 → ρ(770)ρ(770), and D0 → 2(ππ)S are observed in both channels. With the obtained amplitude model, the CP-even fractions of D0 → π+π−π+π− and D0 → π+π−π0π0 (non-η) are determined to be (75.2 ± 1.1stat. ± 1.5syst.) % and (68.9 ± 1.5stat. ± 2.4syst.)%, respectively. The branching fractions of D0 → π+π−π+π− and D0 → π+π−π0π0 (non-η) are measured to be (0.688 ± 0.010stat. ± 0.010syst.)% and (0.951 ± 0.025stat. ± 0.021syst.)%, respectively. The amplitude analysis provides an important model for the binning strategy in measuring the strong phase parameters of D0 → 4π when used to determine the CKM angle γ(ϕ3) via the B− → DK− decay.

AB - Using e+e− annihilation data corresponding to an integrated luminosity of 2.93 fb−1 taken at the center-of-mass energy √s = 3.773 GeV with the BESIII detector, a joint amplitude analysis is performed on the decays D0 → π+π−π+π− and D0 → π+π−π0π0 (non-η). The fit fractions of individual components are obtained, and large interferences among the dominant components of the decays D0 → a1(1260)π, D0 → π(1300)π, D0 → ρ(770)ρ(770), and D0 → 2(ππ)S are observed in both channels. With the obtained amplitude model, the CP-even fractions of D0 → π+π−π+π− and D0 → π+π−π0π0 (non-η) are determined to be (75.2 ± 1.1stat. ± 1.5syst.) % and (68.9 ± 1.5stat. ± 2.4syst.)%, respectively. The branching fractions of D0 → π+π−π+π− and D0 → π+π−π0π0 (non-η) are measured to be (0.688 ± 0.010stat. ± 0.010syst.)% and (0.951 ± 0.025stat. ± 0.021syst.)%, respectively. The amplitude analysis provides an important model for the binning strategy in measuring the strong phase parameters of D0 → 4π when used to determine the CKM angle γ(ϕ3) via the B− → DK− decay.

KW - BESIII

KW - CP-even fraction

KW - D0 meson decays

KW - amplitude analysis

UR - https://www.scopus.com/record/display.uri?eid=2-s2.0-85199341124&origin=inward&txGid=4c56adb4490a591aeb91cac1383e0dc3

U2 - 10.1088/1674-1137/ad3d4d

DO - 10.1088/1674-1137/ad3d4d

M3 - Article

VL - 48

JO - Chinese Physics C

JF - Chinese Physics C

SN - 1674-1137

IS - 8

M1 - 083001

ER -

ID: 62707263