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Observation of a New Excited Beauty Strange Baryon Decaying to Xi(-)(b)pi(+)pi(-)

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Sirunyan, A. M.Tumasyan, A.Adam, W.Andrejkovic, J. W.Bergauer, T.Chatterjee, S.Dragicevic, M.Del Valle, A. EscalanteFruhwirth, R.Jeitler, M.Krammer, N.Lechner, L.Liko, D.Mikulec, IPitters, F. M.Schieck, J.Schofbeck, R.Spanring, M.Templ, S.Waltenberger, W.Wulz, C-EChekhovsky, VLitomin, A.Makarenko, VDarwish, M. R.De Wolf, E. A.Janssen, X.Kello, T.Lelek, A.Sfar, H. RejebVan 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.Muller, D.Sahasransu, A. R.Tavernier, S.Van Doninck, W.Van Mulders, P.Beghin, D.Bilin, B.Clerbaux, B.De Lentdecker, G.Favart, L.Grebenyuk, A.Kalsi, A. K.Lee, K.Mahdavikhorrami, M.Makarenko, IMoureaux, L.Petre, L.Popov, A.Postiau, N.Starling, E.Thomas, L.Vanden Bemden, M.Vander Velde, C.Vanlaer, P.Vannerom, D.Wezenbeek, L.Cornelis, T.Dobur, D.Gruchala, M.Lambrecht, L.Mestdach, G.Niedziela, M.Roskas, C.Skovpen, K.Tran, T. T.Tytgat, M.Verbeke, W.Vermassen, B.Vit, M.Bethani, A.Bruno, G.Bury, F.Caputo, C.David, P.Delaere, C.Donertas, I. S.Giammanco, A.Jaffel, K.Lemaitre, VMondal, K.Prisciandaro, J.Taliercio, A.Teklishyn, M.Vischia, P.Wertz, S.Wuyckens, S.Alves, G. A.Hensel, C.Moraes, A.Alda Junior, W. L.Ferreira Filho, M. BarrosoMalbouisson, H. BrandaoCarvalho, W.Chinellato, J.Da Costa, E. M.Da Silveira, G. G.Damiao, D. De JesusDe Souza, S. FonsecaFigueiredo, D. MatosHerrera, C. MoraAmarilo, K. MotaMundim, L.Nogima, H.Teles, P. RebelloSanchez Rosas, L. J.Santoro, A.Silva Do Amaral, S. M.Sznajder, A.Thiel, M.Da Silva De Araujo, F. TorresPereira, A. VilelaBernardes, C. A.Calligaris, L.Fernandez Perez Tomei, T. R.Gregores, E. M.Lemos, D. S.Mercadante, P. G.Novaes, S. F.Padula, Sandra S.Aleksandrov, A.Antchev, G.Atanasov, IHadjiiska, R.Iaydjiev, P.Misheva, M.Rodozov, M.Shopova, M.Sultanov, G.Dimitrov, A.Ivanov, T.Litov, L.Pavlov, B.Petkov, P.Petrov, A.Cheng, T.Fang, W.Guo, Q.Javaid, T.Mittal, M.Wang, H.Yuan, L.Ahmad, M.Bauer, G.Dozen, C.Hu, Z.Martins, J.Wang, Y.Yi, K.Chapon, E.Chen, G. M.Chen, H. S.Chen, M.Iemmi, F.Kapoor, A.Leggat, D.Liao, H.Liu, Z-ASharma, R.Spiezia, A.Tao, J.Thomas-wilsker, J.Wang, J.Zhang, H.Zhang, S.Zhao, J.Agapitos, A.Ban, Y.Chen, C.Huang, Q.Levin, A.Li, Q.Lu, M.Lyu, X.Mao, Y.Qian, S. J.Wang, D.Wang, Q.Xiao, J.You, Z.Gao, X.Okawa, H.Xiao, M.Avila, C.Cabrera, A.Florez, C.Fraga, J.Sarkar, A.Segura Delgado, M. A.Jaramillo, J.Mejia Guisao, J.Ramirez, F.Ruiz Alvarez, J. D.Salazar Gonzalez, C. 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Issue Date
25-6월-2021
Publisher
AMER PHYSICAL SOC
Citation
PHYSICAL REVIEW LETTERS, v.126, no.25
Indexed
SCIE
SCOPUS
Journal Title
PHYSICAL REVIEW LETTERS
Volume
126
Number
25
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/127822
DOI
10.1103/PhysRevLett.126.252003
ISSN
0031-9007
Abstract
The Xi(-)(b)pi(+)pi(-) invariant mass spectrum is investigated with an event sample of proton-proton collisions at root 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 Xi(-)(b) is reconstructed via its decays to J/psi Xi(-) and J/psi Lambda K-. A narrow resonance, labeled Xi(b)(6100)(-), is observed at a Xi(-)(b)pi(+)pi(-) invariant mass of 6100.3 +/- 0.2(stat) +/- 0.1(syst) +/- 0.6(Xi(-)(b)) MeV, where the last uncertainty reflects the precision of the Xi(-)(b) baryon mass. The upper limit on the Xi(b)(6100)(-) natural width is determined to be 1.9 MeV at 95% confidence level. The low Xi(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 Xi(c) baryon states, the new Xi(b)(6100)(-) resonance and its decay sequence are consistent with the orbitally excited Xi(- )(b)baryon, with spin and parity quantum numbers J(P) = 3/2(-).
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College of Science > Department of Physics > 1. Journal Articles

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