Observation of a Narrow Charmoniumlike State in Exclusive<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msup><mml:mi>B</mml:mi><mml:mo>±</mml:mo></mml:msup><mml:mo>→</mml:mo><mml:msup><mml:mi>K</mml:mi><mml:mo>±</mml:mo></mml:msup><mml:msup><mml:mi>π</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>π</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mi>J</mml:mi><mml:mo>/</mml:mo><mml:mi>ψ</mml:mi></mml:math>Decays

Choi, S. K.; Olsen, S. L.; Abe, K.; Abe, T.; Adachi, I.; Ahn, Byoung Sup; Aihara, H.; Akai, K.; Akatsu, M.; Akemoto, M.; Asano, Y.; Aso, T.; Aulchenko, V.; Aushev, T.; Bakich, A. M.; Ban, Y.; Banerjee, S.; Bondar, A.; Bożek, A.; Bračko, M.; Brodzicka, J.; Browder, T. E.; Chang, P.; Chào, Y.; Chen, K. F.; Cheon, B. G.; Chistov, R.; Choi, Y.; Danilov, M.; Liu, Dong; Drutskoy, A.; Eidelman, S.; Eiges, V.; Flanagan, J.; Fukunaga, C.; Furukawa, K.; Gabyshev, N.; Gershon, T.; Golob, B.; Guler, H.; Guo, R.; Hagner, C.; Handa, F.; Hara, T.; Hastings, N. C.; Hayashii, H.; Hazumi, M.; Hinz, L.; Hoshi, Y.; Hou, W.-S.; Hsiung, Y.; Huang, Hsuan‐Cheng; Iijima, T.; Inami, K.; Ishikawa, A.; Itoh, R.; Iwasaki, M.; Iwasaki, Y.; Kang, J. H.; Kataoka, S. U.; Katayama, N.; Kawai, H.; Kawasaki, T.; Kichimi, H.; Kikutani, E.; Kim, H. J.; Kim, Hyun Woo; Kim, J. H.; Kim, S. K.; Kinoshita, K.; Koiso, H.; Koppenburg, P.; Korpar, S.; Križan, P.; Krokovny, P.; Kumar, Suneel; Kuzmin, A.; Lange, J. S.; Leder, G.; Lee, S. H.; Lesiak, T.; Lin, S. W.; Liventsev, D.; MacNaughton, J.; Majumder, G.; Mandl, F.; Marlow, D.; Matsumoto, T.; Michizono, Shinichiro; Mimashi, T.; Mitaroff, W.; Miyabayashi, K.; Miyake, H.; Mohapatra, D.; Moloney, G. R.; Nagamine, T.; Nagasaka, Y.; Nakadaira, T.; Nakamura, T.; Nakao, M.; Natkaniec, Z.; Nishida, S.; Nitoh, O.; Nozaki, T.; Ogawa, S.; Ogawa, Yoshinori; Ohmi, K.; Ohnishi, Y.; Ohshima, T.; Ohuchi, N.; Oide, K.; Okabe, T.; Okuno, S.; Ostrowicz, W.; Ozaki, H.; Pałka, H.; Park, H.; Parslow, N.; Piilonen, L. E.; Sagawa, H.; Saitoh, Saburou; Sakai, Y.; Sarangi, T.; Satapathy, M.; Satpathy, A.; Schneider, O.; Schwartz, A. J.; Semenov, S.; Senyo, K.; Seuster, R.; Sevior, M. E.; Shibuya, H.; Shidara, T.; Shwartz, B.; Sidorov, V.; Soni, N.; Stanič, S.; Starič, M.; Sugiyama, A.; Sumiyoshi, T.; Suzuki, S.; Takasaki, F.; Tamai, K.; Tamura, N.; Tanaka, M.; Tawada, M.; Taylor, G. N.; Teramoto, Y.; Tomura, T.; Trabelsi, K.; Tsukamoto, T.; Uehara, S.; Ueno, K.; Unno, Y.; Uno, S.; Varner, G.; Varvell, K. E.; Wang, C. C.; Wang, C. H.; Wang, J. G.; Watanabe, Y.; Won, E.; Yabsley, B.; Yamada, Yukiko; Yamaguchi, A.; Yamashita, Y.; Yanai, Haruo; Yang, H. X.; Ying, J.; Yoshida, Masato; Zhang, C. C.; Zhang, Z. P.; Žontar, D.

doi:10.1103/physrevlett.91.262001

Cited by 1,808 publications

(953 citation statements)

References 20 publications

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“…Let's cherish all the expected and embrace all the unexpected. Belle [63], BaBar [84] Belle [75], BaBar [90] Belle [76], BaBar [87] Belle [75], BaBar [86] CDF [67], D0 [68] LHCb [91], CMS [73] LHCb [92] BESIII [93] BaBar [62], CLEO [60], Belle [119] BaBar [123] CLEO [120] BESIII [64], Belle [124] BESIII [159] BESIII [160] BESIII [161] BESIII [93] Belle [172], Belle [177] P c (4380) + * 4380 ± 8 ± 29 [2] 205 ± 18 ± 86 [2] LHCb [2] …”

Section: Discussionmentioning

confidence: 99%

“…in the γχ c1 decay mode in Belle [63], and the upper limit was measured to be Γ(X(3872) → γχ c1 ) Γ(X(3872) → π + π − J/ψ) < 0.89 . Belle [63] 3872 ± 0.6 ± 0.5 < 2. Belle [80] 3871.84 ± 0.27 ± 0.19…”

Section: The Charmonium-like Xyz Statesmentioning

confidence: 99%

“…, and used X u and X d to explain the mass difference between the X(3872) state decaying into J/ψπ + π − [63,90] and the one decaying into D 0D0 π 0 [68]. The quantum numbers of the X(3872), both J PC = 2 −+ and 1 ++ , were discussed by Burns, Piccinini, Polosa, and Sabelli in Ref.…”

Section: Molecular Schemementioning

confidence: 99%

“…• In 2003, the charmonium-like state X(3872) was announced by the Belle Collaboration [63] (see Sec. 2.1.1.1 for its experimental information).…”

Section: +5mentioning

confidence: 99%

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The hidden-charm pentaquark and tetraquark states

et al. 2016

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In the past decade many charmonium-like states were observed experimentally. Especially those charged charmoniumlike Z c states and bottomonium-like Z b states can not be accommodated within the naive quark model. These charged Z c states are good candidates of either the hidden-charm tetraquark states or molecules composed of a pair of charmed mesons. Recently, the LHCb Collaboration discovered two hidden-charm pentaquark states, which are also beyond the quark model. In this work, we review the current experimental progress and investigate various theoretical interpretations of these candidates of the multiquark states. We list the puzzles and theoretical challenges of these models when confronted with the experimental data. We also discuss possible future measurements which may distinguish the theoretical schemes on the underlying structures of the hidden-charm multiquark states.

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Section: Discussionmentioning

confidence: 99%

Section: The Charmonium-like Xyz Statesmentioning

confidence: 99%

Section: Molecular Schemementioning

confidence: 99%

“…• In 2003, the charmonium-like state X(3872) was announced by the Belle Collaboration [63] (see Sec. 2.1.1.1 for its experimental information).…”

Section: +5mentioning

confidence: 99%

See 2 more Smart Citations

The hidden-charm pentaquark and tetraquark states

et al. 2016

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show abstract

“…The missing spin singlet states as well as new, yet to be explained states such as the X(3872) [1], Y(4260) [2], Y(3940) [3] and others have presented a new challenge for the theoretical particle physics community.…”

Section: Introductionmentioning

confidence: 99%

Charmonium spectroscopy on dynamical anisotropic lattices

Juge¹,

Cais²,

Oktay³

et al. 2006

Nuclear Physics B - Proceedings Supplements

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Quarks im Tetrapack

Wiedner

2018

Physik in unserer Zeit

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Zusammenfassung Die starke Wechselwirkung im niederenergetischen Bereich, die sich in der Formation von gebundenen Teilchen darstellt, ist um neue Facetten reicher geworden. Experimente haben Evidenz für Teilchen aus Vier‐ und Fünf‐Quarkzuständen gefunden, die aufgrund ihrer ungewöhnlichen Eigenschaften nicht in das etablierte Baryonen‐ oder Mesonenschema passen. Ihre detaillierte Untersuchung wird unser Wissen über Hadronen, die aus Quarks und Gluonen aufgebaut sind, und deren Wechselwirkung um neue Kapitel erweitern.

show abstract

Observation of a Narrow Charmoniumlike State in ExclusiveB±→K±π+π−J/ψDecays

Cited by 1,808 publications

References 20 publications

The hidden-charm pentaquark and tetraquark states

The hidden-charm pentaquark and tetraquark states

Charmonium spectroscopy on dynamical anisotropic lattices

Quarks im Tetrapack

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