First measurement of the Λc+ → pη′ decay › Обзор исследований

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First measurement of the Λc+ → pη′ decay. / Belle Collaboration.

в: Journal of High Energy Physics, Том 2022, № 3, 90, 03.2022.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Belle Collaboration 2022, 'First measurement of the Λc+ → pη′ decay', Journal of High Energy Physics, Том. 2022, № 3, 90. https://doi.org/10.1007/JHEP03(2022)090

APA

Belle Collaboration (2022). First measurement of the Λc+ → pη′ decay. Journal of High Energy Physics, 2022(3), [90]. https://doi.org/10.1007/JHEP03(2022)090

Vancouver

Belle Collaboration. First measurement of the Λc+ → pη′ decay. Journal of High Energy Physics. 2022 март;2022(3):90. doi: 10.1007/JHEP03(2022)090

Author

Belle Collaboration. / First measurement of the Λc+ → pη′ decay. в: Journal of High Energy Physics. 2022 ; Том 2022, № 3.

BibTeX

@article{bc6a606814bd41969d8ae456b116b980,

title = "First measurement of the Λc+ → pη′ decay",

abstract = "We present the first measurement of the branching fraction of the singly Cabibbo-suppressed (SCS) decay Λc+→ pη′ with η′ → ηπ+π−, using a data sample corresponding to an integrated luminosity of 981 fb−1, collected by the Belle detector at the KEKB e+e− asymmetric-energy collider. A significant Λc+→ pη′ signal is observed for the first time with a signal significance of 5.4σ. The relative branching fraction with respect to the normalization mode Λc+→ pK−π+ is measured to beB(Λc+→pη′)B(Λc+→pK−π+)=(7.54±1.32±0.73)×10−3, where the uncertainties are statistical and systematic, respectively. Using the world-average value of B(Λc+→pK−π+) = (6.28 ± 0.32) × 10−2, we obtainB(Λc+→pη′)=(4.73±0.82±0.46±0.24)×10−4, where the uncertainties are statistical, systematic, and from B(Λc+→pK−π+), respectively.",

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

author = "{The BELLE collaboration} and Li, {S. X.} and Cui, {J. X.} and Shen, {C. P.} and I. Adachi and H. Aihara and {Al Said}, S. and Asner, {D. M.} and H. Atmacan and T. Aushev and R. Ayad and V. Babu and P. Behera and K. Belous and M. Bessner and V. Bhardwaj and B. Bhuyan and T. Bilka and D. Bodrov and G. Bonvicini and J. Borah and A. Bozek and M. Bra{\v c}ko and P. Branchini and Browder, {T. E.} and A. Budano and M. Campajola and D. {\v C}ervenkov and Chang, {M. C.} and P. Chang and V. Chekelian and A. Chen and Cheon, {B. G.} and K. Chilikin and Cho, {H. E.} and K. Cho and Cho, {S. J.} and Choi, {S. K.} and Y. Choi and S. Choudhury and D. Cinabro and S. Cunliffe and D. Epifanov and N. Gabyshev and A. Korobov and E. Kovalenko and P. Krokovny and D. Matvienko and B. Shwartz and A. Vinokurova and V. Zhilich",

note = "Publisher Copyright: {\textcopyright} 2022, The Author(s).",

year = "2022",

month = mar,

doi = "10.1007/JHEP03(2022)090",

language = "English",

volume = "2022",

journal = "Journal of High Energy Physics",

issn = "1029-8479",

publisher = "Springer US",

number = "3",

}

RIS

TY - JOUR

T1 - First measurement of the Λc+ → pη′ decay

AU - The BELLE collaboration

AU - Li, S. X.

AU - Cui, J. X.

AU - Shen, C. P.

AU - Adachi, I.

AU - Aihara, H.

AU - Al Said, S.

AU - Asner, D. M.

AU - Atmacan, H.

AU - Aushev, T.

AU - Ayad, R.

AU - Babu, V.

AU - Behera, P.

AU - Belous, K.

AU - Bessner, M.

AU - Bhardwaj, V.

AU - Bhuyan, B.

AU - Bilka, T.

AU - Bodrov, D.

AU - Bonvicini, G.

AU - Borah, J.

AU - Bozek, A.

AU - Bračko, M.

AU - Branchini, P.

AU - Browder, T. E.

AU - Budano, A.

AU - Campajola, M.

AU - Červenkov, D.

AU - Chang, M. C.

AU - Chang, P.

AU - Chekelian, V.

AU - Chen, A.

AU - Cheon, B. G.

AU - Chilikin, K.

AU - Cho, H. E.

AU - Cho, K.

AU - Cho, S. J.

AU - Choi, S. K.

AU - Choi, Y.

AU - Choudhury, S.

AU - Cinabro, D.

AU - Cunliffe, S.

AU - Epifanov, D.

AU - Gabyshev, N.

AU - Korobov, A.

AU - Kovalenko, E.

AU - Krokovny, P.

AU - Matvienko, D.

AU - Shwartz, B.

AU - Vinokurova, A.

AU - Zhilich, V.

PY - 2022/3

Y1 - 2022/3

N2 - We present the first measurement of the branching fraction of the singly Cabibbo-suppressed (SCS) decay Λc+→ pη′ with η′ → ηπ+π−, using a data sample corresponding to an integrated luminosity of 981 fb−1, collected by the Belle detector at the KEKB e+e− asymmetric-energy collider. A significant Λc+→ pη′ signal is observed for the first time with a signal significance of 5.4σ. The relative branching fraction with respect to the normalization mode Λc+→ pK−π+ is measured to beB(Λc+→pη′)B(Λc+→pK−π+)=(7.54±1.32±0.73)×10−3, where the uncertainties are statistical and systematic, respectively. Using the world-average value of B(Λc+→pK−π+) = (6.28 ± 0.32) × 10−2, we obtainB(Λc+→pη′)=(4.73±0.82±0.46±0.24)×10−4, where the uncertainties are statistical, systematic, and from B(Λc+→pK−π+), respectively.

AB - We present the first measurement of the branching fraction of the singly Cabibbo-suppressed (SCS) decay Λc+→ pη′ with η′ → ηπ+π−, using a data sample corresponding to an integrated luminosity of 981 fb−1, collected by the Belle detector at the KEKB e+e− asymmetric-energy collider. A significant Λc+→ pη′ signal is observed for the first time with a signal significance of 5.4σ. The relative branching fraction with respect to the normalization mode Λc+→ pK−π+ is measured to beB(Λc+→pη′)B(Λc+→pK−π+)=(7.54±1.32±0.73)×10−3, where the uncertainties are statistical and systematic, respectively. Using the world-average value of B(Λc+→pK−π+) = (6.28 ± 0.32) × 10−2, we obtainB(Λc+→pη′)=(4.73±0.82±0.46±0.24)×10−4, where the uncertainties are statistical, systematic, and from B(Λc+→pK−π+), respectively.

KW - Branching fraction

KW - Charm Physics

KW - e-e Experiments

KW - Particle and Resonance Production

UR - http://www.scopus.com/inward/record.url?scp=85133875550&partnerID=8YFLogxK

U2 - 10.1007/JHEP03(2022)090

DO - 10.1007/JHEP03(2022)090

M3 - Article

AN - SCOPUS:85133875550

VL - 2022

JO - Journal of High Energy Physics

JF - Journal of High Energy Physics

SN - 1029-8479

IS - 3

M1 - 90

ER -

ID: 36704296