Observation of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mo stretchy="false">→</mml:mo><mml:mi>γ</mml:mi><mml:mi>X</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>3872</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math>at BESIII

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doi:10.1103/physrevlett.112.092001

Cited by 384 publications

(765 citation statements)

References 27 publications

Supporting

Mentioning

713

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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%

“…[93], the BESIII Collaboration studied the e + e − → γX(3872) process and measured the product of the cross section σ(e + e − → γX(3872)) and the branching ratio B(X(3872) → π + π − J/ψ) at center-of-mass energies 4.009, 4.229, 4.26 and 4.360 GeV, which hinted the existence of the Y(4260) → γX(3872) radiative decay. More experimental information is needed to confirm the Y(4260) → γX(3872) mode.…”

Section: Its Open Charm Decay Modesmentioning

confidence: 99%

“…BaBar [85] 3871.3 ± 0.6 ± 0.1 BESIII [93] 3871.9 ± 0.7 ± 0.2 < 2.4 e + e − [→ Y(4260)] → γX(→ π + π − J/ψ) Table 2: Some product branching fractions of the X(3872) resonance. Here, the X(3872) is abbreviated as X.…”

Section: The Charmonium-like Xyz Statesmentioning

confidence: 99%

See 2 more Smart Citations

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.

show abstract

Section: Discussionmentioning

confidence: 99%

Section: Its Open Charm Decay Modesmentioning

confidence: 99%

See 1 more Smart Citation

The hidden-charm pentaquark and tetraquark states

et al. 2016

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show abstract

“…X(3872), the well-known one of the XY Z particles [77], is supposed to χ ′ c1 state or the mixture of this state with other structure in some view [49,78]. Recently, X(3872) has been observed in photon-recoiled process with a statistical significance of 6.4σ at BESIII [79]. X(3915) (X(3945) or Y (3940)) and Z(3930) are assigned as χ c0 (2P ) and χ c2 (2P ) states by the Particle Data Group (PDG) [80], however this identification may call into some questions [81].…”

Section: Jhep10(2014)071mentioning

confidence: 99%

α s v 2 corrections to η c and χ cJ production recoiled with a photon at e + e − colliders

Liu

et al. 2014

J. High Energ. Phys.

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“…BESIII observed e + e − → γX(3872) → γπ + π − J/ψ, with J/ψ reconstructed through its decays into lepton pairs ( + − = e + e − or μ + μ − ) [16].The M(π + π − J/ψ) distribution (summed over all energy points), as shown in Fig. 5 (left), was fitted to extract the mass and signal yield of X(3872).…”

Section: Observation Of Y(4260) → γX(3872)mentioning

confidence: 99%

Recent results on hadron spectroscopy from BESIII

Liu¹

2016

AIP Conference Proceedings

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Abstract. Hadron spectroscopy is one of the most important physics goals of BESIII. BESIII brings great opportunities to study the XYZ states of charmonium by directly producing the Y states up to 4.6 GeV. High statistics of charmonium decays collected at BESIII provide an excellent place for hunting gluonic excitations and studying the excited baryons. Recent results of light hadron spectroscopy and charmonium spectroscopy from BESIII will be reported.

show abstract

Observation ofe+e−→γX(3872)at BESIII

Cited by 384 publications

References 27 publications

The hidden-charm pentaquark and tetraquark states

The hidden-charm pentaquark and tetraquark states

α s v 2 corrections to η c and χ cJ production recoiled with a photon at e + e − colliders

Recent results on hadron spectroscopy from BESIII

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