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Observation of a New Excited Beauty Strange Baryon Decaying to Ξ_{b}
Sirunyan, A M; Tumasyan, A; Adam, W; Andrejkovic, J W; Bergauer, T; Chatterjee, S; Dragicevic, M; Escalante Del Valle, A; Frühwirth, R; Jeitler, M; Krammer, N; Lechner, L; Liko, D; Mikulec, I; Pitters, F M; Schieck, J; Schöfbeck, R; Spanring, M; Templ, S; Waltenberger, W; Wulz, C-E; Chekhovsky, V; Litomin, A; Makarenko, V; Darwish, M R; De Wolf, E A; Janssen, X; Kello, T; Lelek, A; Rejeb Sfar, H; Van Mechelen, P; Van Putte, S; Van Remortel, N; Blekman, F; Bols, E S; D'Hondt, J; De Clercq, J; Delcourt, M; Lowette, S; Moortgat, S; Morton, A; Müller, D; Sahasransu, A R; Tavernier, S; Van Doninck, W; Van Mulders, P; Beghin, D; Bilin, B; Clerbaux, B; De Lentdecker, G.
Afiliação
  • Sirunyan AM; Yerevan Physics Institute, Yerevan, Armenia.
  • Tumasyan A; Yerevan Physics Institute, Yerevan, Armenia.
  • Adam W; Institut für Hochenergiephysik, Wien, Austria.
  • Andrejkovic JW; Institut für Hochenergiephysik, Wien, Austria.
  • Bergauer T; Institut für Hochenergiephysik, Wien, Austria.
  • Chatterjee S; Institut für Hochenergiephysik, Wien, Austria.
  • Dragicevic M; Institut für Hochenergiephysik, Wien, Austria.
  • Escalante Del Valle A; Institut für Hochenergiephysik, Wien, Austria.
  • Frühwirth R; Institut für Hochenergiephysik, Wien, Austria.
  • Jeitler M; Institut für Hochenergiephysik, Wien, Austria.
  • Krammer N; Institut für Hochenergiephysik, Wien, Austria.
  • Lechner L; Institut für Hochenergiephysik, Wien, Austria.
  • Liko D; Institut für Hochenergiephysik, Wien, Austria.
  • Mikulec I; Institut für Hochenergiephysik, Wien, Austria.
  • Pitters FM; Institut für Hochenergiephysik, Wien, Austria.
  • Schieck J; Institut für Hochenergiephysik, Wien, Austria.
  • Schöfbeck R; Institut für Hochenergiephysik, Wien, Austria.
  • Spanring M; Institut für Hochenergiephysik, Wien, Austria.
  • Templ S; Institut für Hochenergiephysik, Wien, Austria.
  • Waltenberger W; Institut für Hochenergiephysik, Wien, Austria.
  • Wulz CE; Institut für Hochenergiephysik, Wien, Austria.
  • Chekhovsky V; Institute for Nuclear Problems, Minsk, Belarus.
  • Litomin A; Institute for Nuclear Problems, Minsk, Belarus.
  • Makarenko V; Institute for Nuclear Problems, Minsk, Belarus.
  • Darwish MR; Universiteit Antwerpen, Antwerpen, Belgium.
  • De Wolf EA; Universiteit Antwerpen, Antwerpen, Belgium.
  • Janssen X; Universiteit Antwerpen, Antwerpen, Belgium.
  • Kello T; Universiteit Antwerpen, Antwerpen, Belgium.
  • Lelek A; Universiteit Antwerpen, Antwerpen, Belgium.
  • Rejeb Sfar H; Universiteit Antwerpen, Antwerpen, Belgium.
  • Van Mechelen P; Universiteit Antwerpen, Antwerpen, Belgium.
  • Van Putte S; Universiteit Antwerpen, Antwerpen, Belgium.
  • Van Remortel N; Universiteit Antwerpen, Antwerpen, Belgium.
  • Blekman F; Vrije Universiteit Brussel, Brussel, Belgium.
  • Bols ES; Vrije Universiteit Brussel, Brussel, Belgium.
  • D'Hondt J; Vrije Universiteit Brussel, Brussel, Belgium.
  • De Clercq J; Vrije Universiteit Brussel, Brussel, Belgium.
  • Delcourt M; Vrije Universiteit Brussel, Brussel, Belgium.
  • Lowette S; Vrije Universiteit Brussel, Brussel, Belgium.
  • Moortgat S; Vrije Universiteit Brussel, Brussel, Belgium.
  • Morton A; Vrije Universiteit Brussel, Brussel, Belgium.
  • Müller D; Vrije Universiteit Brussel, Brussel, Belgium.
  • Sahasransu AR; Vrije Universiteit Brussel, Brussel, Belgium.
  • Tavernier S; Vrije Universiteit Brussel, Brussel, Belgium.
  • Van Doninck W; Vrije Universiteit Brussel, Brussel, Belgium.
  • Van Mulders P; Vrije Universiteit Brussel, Brussel, Belgium.
  • Beghin D; Université Libre de Bruxelles, Bruxelles, Belgium.
  • Bilin B; Université Libre de Bruxelles, Bruxelles, Belgium.
  • Clerbaux B; Université Libre de Bruxelles, Bruxelles, Belgium.
  • De Lentdecker G; Université Libre de Bruxelles, Bruxelles, Belgium.
Phys Rev Lett ; 126(25): 252003, 2021 Jun 25.
Article em En | MEDLINE | ID: mdl-34241504
ABSTRACT
The Ξ_{b}^{-}π^{+}π^{-} invariant mass spectrum is investigated with an event sample of proton-proton collisions at sqrt[s]=13 TeV, collected by the CMS experiment at the LHC in 2016-2018 and corresponding to an integrated luminosity of 140 fb^{-1}. The ground state Ξ_{b}^{-} is reconstructed via its decays to J/ψΞ^{-} and J/ψΛK^{-}. A narrow resonance, labeled Ξ_{b}(6100)^{-}, is observed at a Ξ_{b}^{-}π^{+}π^{-} invariant mass of 6100.3±0.2(stat)±0.1(syst)±0.6(Ξ_{b}^{-}) MeV, where the last uncertainty reflects the precision of the Ξ_{b}^{-} baryon mass. The upper limit on the Ξ_{b}(6100)^{-} natural width is determined to be 1.9 MeV at 95% confidence level. The low Ξ_{b}(6100)^{-} signal yield observed in data does not allow a measurement of the quantum numbers of the new state. However, following analogies with the established excited Ξ_{c} baryon states, the new Ξ_{b}(6100)^{-} resonance and its decay sequence are consistent with the orbitally excited Ξ_{b}^{-} baryon, with spin and parity quantum numbers J^{P}=3/2^{-}.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2021 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2021 Tipo de documento: Article