Observation of the Narrow State<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>X</mml:mi><mml:mo>(</mml:mo><mml:mn>3872</mml:mn><mml:mo>)</mml:mo><mml:mo>→</mml:mo><mml:mi>J</mml:mi><mml:mo>/</mml:mo><mml:mi>ψ</mml:mi><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:math>in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mover accent="true"><mml:mi>p</mml:mi><mml:mo>¯</mml:

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L.; Cabrera, S.; Calafiura, P.; Campanelli, M.; Campbell, M.; Canepa, A.; Carlsmith, D.; Carron, S.; Carosi, R.; Casarsa, M.; Castro, A.; Catastini, P.; Cauz, D.; Cerri, A.; Cerri, C.; Cerrito, L.; Chapman, J.; Chen, C.; Chen, Y. C.; Chertok, M.; Chiarelli, G.; Chlachidze, G.; Chlebana, F.; Cho, K.; Chokheli, D.; Chu, M. L.; Chung, J. Y.; Chung, W. H.; Chung, Y. S.; Ciobanu, C. I.; Ciocci, M. A.; Clark, A.; Clark, D.; Coca, M.; Connolly, A.; Convery, M. E.; Conway, J.; Cordelli, M.; Cortiana, G.; Cranshaw, J.; Culbertson, R.; Currat, C.; Cyr, D.; Dagenhart, D.; DaRonco, S.; D’Auria, S.; Barbaro, P. de; Cecco, S. De; Lentdecker, G. De; Dell’Agnello, S.; Dell’Orso, M.; Demers, S.; Demortier, L.; Deninno, M.; Pedis, D. De; Derwent, P. F.; Dionisi, C.; Dittmann, J.; Doksus, P.; Dominguez, A.; Donati, S.; D’Onofrio, M.; Dorigo, T.; Drollinger, V.; Ebina, K.; Eddy, N.; Ely, R.; Erbacher, R.; Erdmann, M.; Errede, D.; Errede, S.; Eusebi, R.; Fang, H. C.; Farrington, S. 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L.; Wagner, W.; Wallace, N. B.; Walter, T.; Zhang, Wan; Wang, M. J.; Wang, S. M.; Warburton, A.; Ward, B. F. L.; Waschke, S.; Waters, D.; Watts, T.; Weber, M.; Wester, W. C.; Whitehouse, B.; Wicklund, A. B.; Wicklund, E.; Williams, H. H.; Wilson, P.; Winer, B. L.; Wittich, P.; Wolbers, S.; Wolter, M. W.; Worcester, M.; Worm, S. D.; Wright, T.; Wu, X.; Würthwein, F.; Wyatt, A.; Yagil, A.; Yamashita, T.; Yamamoto, K.; Yang, U. K.; Yao, W-M.; Yeh, G. P.; Yi, K.; Yoh, J.; Yoon, P.; Yorita, K.; Yoshida, T.; Yu, I.; Yu, S. S.; Z, Yu; Yun, J. C.; Zanello, L.; Zanetti, A.; Zaw, I.; Zetti, F.; Zhou, J.; Žsenei, A.; Zucchelli, S.

doi:10.1103/physrevlett.93.072001

Cited by 592 publications

(194 citation statements)

References 18 publications

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“…confirmed later in some other experiments [2][3][4]. The exotic states were produced and observed in B meson decays, in the e + e − and pp annihilations, in the double charmonium production processes, in the two-photon fusion and pp collisions.…”

Section: Introductionsupporting

confidence: 58%

“…Later the X(3872) was observed also through direct production mode in pp annihilation [2,3], as well as in the e + e − annihilation and pp collisions [13]. The assigned quantum numbers to X state are 1 ++ , its average mass extracted from different experiments is m X = (3871.69 ± 0.17) MeV , and the decay width was estimated as Γ < 1.2 MeV [10,19,20].…”

Section: Introductionmentioning

confidence: 99%

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The Mass and Current-Meson Coupling Constant of the Exotic X(3872) State from QCD Sum Rules

Sundu

2016

SDÜ Fen Bil Enst Der

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Abstract:The mass and current-meson coupling constant of the exotic X(3872) state are computed within the two-point sum rule method using the diquark-antidiquark and molecule interpolating currents. In calculations the quark, gluon and mixed vacuum condensates up to ten dimensions are taken into account. Within the diquark-antidiquark picture for the mass of the X(3872) state we obtain m X = 3873 MeV , which is very close to the experimental result of the Belle Collaboration. The molecule model leads for m X to the prediction that slightly exceeds the experimental data. We compare our predictions for the mass and coupling constant with available experimental data and other theoretical results. KRD Toplam Kurallarında Ekzotik X(3872) Durumunun Kütle ve Akım-Mezon Kuplaj SabitiAnahtar Kelimeler Ekzotik hadron, KRD toplam kuralları, Kütle, Akım-Mezon kuplaj sabiti Özet: Ekzotik X(3872) durumunun kütle ve akım-mezon kuplaj sabiti, dikuarkantidikuark ve molekül arakesit akımları kullanılarak iki-nokta toplam kuralları metodu ile hesaplanmıştır. Hesaplamalarda, on boyuta kadar kuark, gluon ve birleşik vakum kondensatları göz önüne alınmıştır. Dikuark-antidikuark akım çerçevesinde X(3872) durumunun kütlesi için, Belleİşbirliginin deneysel sonucu ile oldukça yakın olan m X = 3873 MeV degeri elde edilmiştir. Molekül model, m X öngörüsü için deneysel sonucu kısmen aştıgını ileri sürmektedir. Kütle ve kuplaj sabiti için elde edilen sonuçlar deney dataları ve diger teorik sonuçlar ile karşılaştırılmıştır.

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Section: Introductionsupporting

confidence: 58%

Section: Introductionmentioning

confidence: 99%

The Mass and Current-Meson Coupling Constant of the Exotic X(3872) State from QCD Sum Rules

Sundu

2016

SDÜ Fen Bil Enst Der

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“…The efficiency is calculated for the 2011a dataset in each bin since the changes in efficiency related to the trigger evolution during data taking do not affect the efficiency ratio. The average value of A · in each p T bin is determined using fine-grained bins in transverse momentum as 3) where N i is the number of signal events observed in the data,…”

Section: Jhep04(2013)154mentioning

confidence: 99%

“…The discovery of the X(3872) resonance by the Belle experiment in 2003 [1] and its subsequent confirmation by BaBar, CDF, and D0 [2][3][4] has attracted a large interest in "exotic" quarkonium spectroscopy since it was the first observation of an unexpected charmonium candidate. Many new unconventional states with masses above the open-charm or open-bottom thresholds, m > m(DD) and m > m(BB), respectively, have been observed [5].…”

Section: Introductionmentioning

confidence: 99%

Measurement of the X(3872) production cross section via decays to J/ψπ + π − in pp collisions at $ \sqrt{s}=7 $ TeV

Chatrchyan

Khachatryan

Sirunyan

et al. 2013

J. High Energ. Phys.

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Measurement of the X(3872) production cross section via decays to J/ψπ + π − in pp collisions at √ s = 7 TeVThe CMS collaboration E-mail: cms-publication-committee-chair@cern.chAbstract: The production of the X(3872) is studied in pp collisions at √ s = 7 TeV, using decays to J/ψπ + π − , where the J/ψ decays to two muons. The data were recorded by the CMS experiment and correspond to an integrated luminosity of 4.8 fb −1 . The measurements are performed in a kinematic range in which the X(3872) candidates have a transverse momentum 10 < p T < 50 GeV and rapidity |y| < 1.2. The ratio of the X(3872) and ψ(2S) cross sections times their branching fractions into J/ψπ + π − is measured as a function of p T . In addition, the fraction of X(3872) originating from B decays is determined. From these measurements the prompt X(3872) differential cross section times branching fraction as a function of p T is extracted. The π + π − mass spectrum of the J/ψπ + π − system in the X(3872) decays is also investigated.

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“…Decays of B mesons provide a fruitful opportunity to study these states and to find new ones. For example, the state X(3872) was first observed by Belle in exclusive B + → K + π + π − J/ψ decays [1] that was later confirmed by CDF [2], DØ [3] and BaBar [4]. It was also observed in the LHCb experiment [5,6] in pp collisions and B decays.…”

Section: Introductionmentioning

confidence: 67%

Search for B decays to final states with the η c meson

Vinokurova¹,

Kuzmin²,

Eidelman³

et al. 2015

J. High Energ. Phys.

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We report a search for B decays to selected final states with the η c meson:The analysis is based on 772 × 10 6 BB pairs collected at the Υ(4S) resonance with the Belle detector at the KEKB asymmetric-energy e + e − collider. We set 90% confidence level upper limits on the branching fractions of the studied B decay modes, independent of intermediate resonances, in the range (0.6-5.3) × 10 −4 . We also search for molecular-state candidates in the D 0D * 0 −D 0 D * 0 , D 0D0 +D 0 D 0 and D * 0D * 0 +D * 0 D * 0 combinations, neutral partners of the Z(3900) ± and Z(4020) ± , and a poorly understood state X(3915) as possible intermediate states in the decay chain, and set 90% confidence level upper limits on the product of branching fractions to the mentioned intermediate states and decay branching fractions of these states in the range (0.6-6.9) × 10 −5 .

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Observation of the Narrow StateX(3872)→J/ψπ+π−inp¯

Cited by 592 publications

References 18 publications

The Mass and Current-Meson Coupling Constant of the Exotic X(3872) State from QCD Sum Rules

The Mass and Current-Meson Coupling Constant of the Exotic X(3872) State from QCD Sum Rules

Measurement of the X(3872) production cross section via decays to J/ψπ + π − in pp collisions at $ \sqrt{s}=7 $ TeV

Search for B decays to final states with the η c meson

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