Artículo

Measurements of ψ(2S) and X(3872)→J/ψπ+π− production in pp collisions at s√=8 TeV with the ATLAS detector

Aaboud, M. ; Aad, G. ; Abbott, B. ; Abdallah, J. ; Abdinov, O. ; Alconada Verzini, María Josefina Icon; Alonso, Francisco Icon; Arduh, Francisco Anuar Icon; Dova, Maria Teresa Icon; Hoya, Joaquín Icon; Monticelli, Fernando Gabriel Icon; Wahlberg, Hernan Pablo Icon; Bossio Sola, Jonathan David Icon; Marceca, Gino Icon; Otero y Garzon, Gustavo Javier Icon; Piegaia, Ricardo Nestor Icon; Sacerdoti, Sabrina Icon; Zibell. A. ; Zieminska, D. ; Zimine, N. I. ; Zimmermann, C. ; Zimmermann, S. ; Zinonos, Z. ; Zinser, M. ; Ziolkowski, M. ; Živković, L. ; Zobernig, G. ; Zoccoli, A. ; Nedden, M. zur ; Zurzolo, G. ; Zwalinski, L. ; The ATLAS Collaboration

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Fecha

10/2016

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Springer

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Journal of High Energy Physics

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1126-6708

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Inglés

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Resumen

Differential cross sections are presented for the prompt and non-prompt production of the hidden-charm states X(3872) and ψ(2S ), in the decay mode J/ψπ+π − , measured using 11.4 fb−1 of pp collisions at √ s = 8 TeV by the ATLAS detector at the LHC. The ratio of cross-sections X(3872)/ψ(2S ) is also given, separately for prompt and non-prompt components, as well as the non-prompt fractions of X(3872) and ψ(2S ). Assuming independent single effective lifetimes for non-prompt X(3872) and ψ(2S ) production gives RB = B(B→X(3872) + any)B(X(3872)→J/ψπ+π − ) B(B→ψ(2S ) + any)B(ψ(2S )→J/ψπ+π −) = (3.95 ± 0.32(stat) ± 0.08(sys)) × 10−2 , while separating short- and long-lived contributions, assuming that the short-lived component is due to Bc decays, gives RB = (3.57 ± 0.33(stat) ± 0.11(sys)) × 10−2 , with the fraction of non-prompt X(3872) produced via Bc decays for pT(X(3872)) > 10 GeV being (25 ± 13(stat) ± 2(sys) ± 5(spin))%. The distributions of the dipion invariant mass in the X(3872) and ψ(2S ) decays are also measured and compared to theoretical predictions

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