Abstract:Charmonium, the spectroscopy of cc mesons, has recently enjoyed a renaissance with the discovery of several missing states and a number of unexpected charmonium-like resonances. The discovery of these new states has been made possible by the extremely large data samples made available by the B-factories at the Stanford Linear Accelerator Center and at KEK in Japan, and at the CESR e + e − collider at Cornell. Conventional cc states are well described by quark potential models. However, many of these newly disc… Show more
“…Indeed, for a charmonium state with J P C = 0 −+ (η c ) the mass is a little low and for J P C = 0 ++ (χ ′ c0 ) the mass is too high [20], also if it had a simple cc structure one would expect that the open charm decay modes would be dominant, and the other, ωJ/ψ, negligible. Also, the large partial width Y (3940) → ωJ/ψ, estimated above 1 MeV [21], is quite larger than the measured partial widths for any of the observed hadronic transitions between charmonium states.…”
Section: Introductionmentioning
confidence: 56%
“…In the production process the two photons can only produce DD in a 0 ++ or 2 ++ states. The Belle measurements favors the 2 ++ hypothesis, making the assignment of the Z(3930) to the 2 3 P 2 (χ ′ c2 ) charmonium state possible [21], following the arguments given in [27]. In this paper we will propose a theoretical explanation on the nature of some of these XYZ states, providing structure and quantum numbers for them.…”
The Y (3940), Z(3930) and the X(4160) as dynamically generated resonances from the vector-vector interaction Abstract We study the vector-vector interaction within the framework of the hidden gauge formalism for the channels with quantum numbers Charm C = 0 and Strangeness S = 0 in the energy region around 4000 MeV. By looking for poles in the complex plane we find three resonances that could be identified by the mass, width and quantum numbers with the Y (3940), Z(3940) and X(4160), these poles appear with isospin I = 0 and J P C = 0 ++ , 2 ++ and 2 ++ respectively. Whereas the Y (3940) and Z(3940) are coupled more strongly to D * D * , the X(4160) is basically a D * sD * s molecular state. Another two extra resonances appear in our approach with I = 0, 1 and J P C = 1 +− , 2 ++ which are not found in the PDG with masses M = 3945, 3912 MeV and widths Γ = 0, 120 MeV respectively.
“…Indeed, for a charmonium state with J P C = 0 −+ (η c ) the mass is a little low and for J P C = 0 ++ (χ ′ c0 ) the mass is too high [20], also if it had a simple cc structure one would expect that the open charm decay modes would be dominant, and the other, ωJ/ψ, negligible. Also, the large partial width Y (3940) → ωJ/ψ, estimated above 1 MeV [21], is quite larger than the measured partial widths for any of the observed hadronic transitions between charmonium states.…”
Section: Introductionmentioning
confidence: 56%
“…In the production process the two photons can only produce DD in a 0 ++ or 2 ++ states. The Belle measurements favors the 2 ++ hypothesis, making the assignment of the Z(3930) to the 2 3 P 2 (χ ′ c2 ) charmonium state possible [21], following the arguments given in [27]. In this paper we will propose a theoretical explanation on the nature of some of these XYZ states, providing structure and quantum numbers for them.…”
The Y (3940), Z(3930) and the X(4160) as dynamically generated resonances from the vector-vector interaction Abstract We study the vector-vector interaction within the framework of the hidden gauge formalism for the channels with quantum numbers Charm C = 0 and Strangeness S = 0 in the energy region around 4000 MeV. By looking for poles in the complex plane we find three resonances that could be identified by the mass, width and quantum numbers with the Y (3940), Z(3940) and X(4160), these poles appear with isospin I = 0 and J P C = 0 ++ , 2 ++ and 2 ++ respectively. Whereas the Y (3940) and Z(3940) are coupled more strongly to D * D * , the X(4160) is basically a D * sD * s molecular state. Another two extra resonances appear in our approach with I = 0, 1 and J P C = 1 +− , 2 ++ which are not found in the PDG with masses M = 3945, 3912 MeV and widths Γ = 0, 120 MeV respectively.
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.
“…Most of them cannot be described well by quarkonium potential models and may be the good candidates of exotic states [1,2,3]. Their unusual properties have stimulated considerable theoretical interest and various interpretations have been proposed, including tetraquarks, molecules, hybrids, or hadrocharmonia [1,3,4].…”
Many hadronic states beyond the conventional quark model (called charmoniumlike/bottomoniumlike states or XY Z particles) were found during the past fourteen years. Their nature properties were proposed including glueballs, hybrids, multi-quark states, hadron molecules, etc. In this report, I present the most recent results on the XY Z results from some experiments.
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