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Test of CP Symmetry in Hyperon to Neutron Decays. / BESIII Collaboration ; Мучной, Николай Юрьевич.

In: Physical Review Letters, Vol. 131, No. 19, 10.11.2023, p. 191802.

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BESIII Collaboration & Мучной, НЮ 2023, 'Test of CP Symmetry in Hyperon to Neutron Decays', Physical Review Letters, vol. 131, no. 19, pp. 191802. https://doi.org/10.1103/PhysRevLett.131.191802

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Vancouver

BESIII Collaboration, Мучной НЮ. Test of CP Symmetry in Hyperon to Neutron Decays. Physical Review Letters. 2023 Nov 10;131(19):191802. doi: 10.1103/PhysRevLett.131.191802

Author

BESIII Collaboration ; Мучной, Николай Юрьевич. / Test of CP Symmetry in Hyperon to Neutron Decays. In: Physical Review Letters. 2023 ; Vol. 131, No. 19. pp. 191802.

BibTeX

@article{55fb9c8e2e9b471eae7008f95255d280,
title = "Test of CP Symmetry in Hyperon to Neutron Decays",
abstract = "The quantum entangled J/ψ→Σ^{+}Σ[over ¯]^{-} pairs from (1.0087±0.0044)×10^{10}  J/ψ events taken by the BESIII detector are used to study the nonleptonic two-body weak decays Σ^{+}→nπ^{+} and Σ[over ¯]^{-}→n[over ¯]π^{-}. The CP-odd weak decay parameters of the decays Σ^{+}→nπ^{+} (α_{+}) and Σ[over ¯]^{-}→n[over ¯]π^{-} (α[over ¯]_{-}) are determined to be 0.0481±0.0031_{stat}±0.0019_{syst} and -0.0565±0.0047_{stat}±0.0022_{syst}, respectively. The decay parameter α[over ¯]_{-} is measured for the first time, and the accuracy of α_{+} is improved by a factor of 4 compared to the previous results. The simultaneously determined decay parameters allow the first precision CP symmetry test for any hyperon decay with a neutron in the final state with the measurement of A_{CP}=(α_{+}+α[over ¯]_{-})/(α_{+}-α[over ¯]_{-})=-0.080±0.052_{stat}±0.028_{syst}. Assuming CP conservation, the average decay parameter is determined as ⟨α_{+}⟩=(α_{+}-α[over ¯]_{-})/2=-0.0506±0.0026_{stat}±0.0019_{syst}, while the ratios α_{+}/α_{0} and α[over ¯]_{-}/α[over ¯]_{0} are -0.0490±0.0032_{stat}±0.0021_{syst} and -0.0571±0.0053_{stat}±0.0032_{syst}, where α_{0} and α[over ¯]_{0} are the decay parameters of the decays Σ^{+}→pπ^{0} and Σ[over ¯]^{-}→p[over ¯]π^{0}, respectively.",
author = "{BESIII Collaboration} and Achasov, {M N} and C Chen and Nikolaev, {I B} and Мучной, {Николай Юрьевич}",
note = "Test of CP Symmetry in Hyperon to Neutron Decays / BESIII Collaboration // Physical Review Letters. – 2023. – Vol. 131, No. 19. – P. 191802. – DOI 10.1103/physrevlett.131.191802.",
year = "2023",
month = nov,
day = "10",
doi = "10.1103/PhysRevLett.131.191802",
language = "English",
volume = "131",
pages = "191802",
journal = "Physical Review Letters",
issn = "0031-9007",
publisher = "American Physical Society",
number = "19",

}

RIS

TY - JOUR

T1 - Test of CP Symmetry in Hyperon to Neutron Decays

AU - BESIII Collaboration

AU - Achasov, M N

AU - Chen, C

AU - Nikolaev, I B

AU - Мучной, Николай Юрьевич

N1 - Test of CP Symmetry in Hyperon to Neutron Decays / BESIII Collaboration // Physical Review Letters. – 2023. – Vol. 131, No. 19. – P. 191802. – DOI 10.1103/physrevlett.131.191802.

PY - 2023/11/10

Y1 - 2023/11/10

N2 - The quantum entangled J/ψ→Σ^{+}Σ[over ¯]^{-} pairs from (1.0087±0.0044)×10^{10}  J/ψ events taken by the BESIII detector are used to study the nonleptonic two-body weak decays Σ^{+}→nπ^{+} and Σ[over ¯]^{-}→n[over ¯]π^{-}. The CP-odd weak decay parameters of the decays Σ^{+}→nπ^{+} (α_{+}) and Σ[over ¯]^{-}→n[over ¯]π^{-} (α[over ¯]_{-}) are determined to be 0.0481±0.0031_{stat}±0.0019_{syst} and -0.0565±0.0047_{stat}±0.0022_{syst}, respectively. The decay parameter α[over ¯]_{-} is measured for the first time, and the accuracy of α_{+} is improved by a factor of 4 compared to the previous results. The simultaneously determined decay parameters allow the first precision CP symmetry test for any hyperon decay with a neutron in the final state with the measurement of A_{CP}=(α_{+}+α[over ¯]_{-})/(α_{+}-α[over ¯]_{-})=-0.080±0.052_{stat}±0.028_{syst}. Assuming CP conservation, the average decay parameter is determined as ⟨α_{+}⟩=(α_{+}-α[over ¯]_{-})/2=-0.0506±0.0026_{stat}±0.0019_{syst}, while the ratios α_{+}/α_{0} and α[over ¯]_{-}/α[over ¯]_{0} are -0.0490±0.0032_{stat}±0.0021_{syst} and -0.0571±0.0053_{stat}±0.0032_{syst}, where α_{0} and α[over ¯]_{0} are the decay parameters of the decays Σ^{+}→pπ^{0} and Σ[over ¯]^{-}→p[over ¯]π^{0}, respectively.

AB - The quantum entangled J/ψ→Σ^{+}Σ[over ¯]^{-} pairs from (1.0087±0.0044)×10^{10}  J/ψ events taken by the BESIII detector are used to study the nonleptonic two-body weak decays Σ^{+}→nπ^{+} and Σ[over ¯]^{-}→n[over ¯]π^{-}. The CP-odd weak decay parameters of the decays Σ^{+}→nπ^{+} (α_{+}) and Σ[over ¯]^{-}→n[over ¯]π^{-} (α[over ¯]_{-}) are determined to be 0.0481±0.0031_{stat}±0.0019_{syst} and -0.0565±0.0047_{stat}±0.0022_{syst}, respectively. The decay parameter α[over ¯]_{-} is measured for the first time, and the accuracy of α_{+} is improved by a factor of 4 compared to the previous results. The simultaneously determined decay parameters allow the first precision CP symmetry test for any hyperon decay with a neutron in the final state with the measurement of A_{CP}=(α_{+}+α[over ¯]_{-})/(α_{+}-α[over ¯]_{-})=-0.080±0.052_{stat}±0.028_{syst}. Assuming CP conservation, the average decay parameter is determined as ⟨α_{+}⟩=(α_{+}-α[over ¯]_{-})/2=-0.0506±0.0026_{stat}±0.0019_{syst}, while the ratios α_{+}/α_{0} and α[over ¯]_{-}/α[over ¯]_{0} are -0.0490±0.0032_{stat}±0.0021_{syst} and -0.0571±0.0053_{stat}±0.0032_{syst}, where α_{0} and α[over ¯]_{0} are the decay parameters of the decays Σ^{+}→pπ^{0} and Σ[over ¯]^{-}→p[over ¯]π^{0}, respectively.

UR - https://pubmed.ncbi.nlm.nih.gov/38000397/

UR - https://www.elibrary.ru/item.asp?id=64206243

U2 - 10.1103/PhysRevLett.131.191802

DO - 10.1103/PhysRevLett.131.191802

M3 - Article

C2 - 38000397

VL - 131

SP - 191802

JO - Physical Review Letters

JF - Physical Review Letters

SN - 0031-9007

IS - 19

ER -

ID: 68340086