Investigating different structures of the Z_{b}(10610) and Z_{b}(10650)
arXiv:1107.1343 · doi:10.1103/PhysRevD.85.074014
Abstract
The recently observed narrow resonance is examined with the assumptions both as a molecular state and a tetraquark state with quantum numbers . Possible interpolating currents are constructed to describe the as an axial-vector molecular state or a tetraquark state. Using QCD sum rules (QCDSR), we consider contributions up to dimension six in the operator product expansion (OPE) at the leading order in . The mass is obtained as for molecular state and for tetraquark state, both of which coincide with the . The results and are consistent with the .
17 pages, 9 figures
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Cited by in corpus (38)
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- Bottomonium spectrum revisited
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- Exotic mesons with hidden bottom near thresholds
- Decays of Zb(+) and Zb'(+) as hadronic molecules
- Study of and interactions in and relationship to the , states
- Possible interpretation of the (10610) and (10650) in a chiral quark model
- General considerations on the nature of and from their pole positions
- Interpretation of as the Hidden Charm Tetraquark States via QCD Sum Rules
- and decays in intermediate meson loops model
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- Line shapes in Υ(5S) \to B^{(*)} \bar{B}^{(*)}πwith Z(10610) and Z(10650) using effective field theory
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- Light baryonium spectrum
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- Magnetic dipole moment of in light-cone QCD
- Decays of Zb -> Upsilon + pi via triangle diagrams in heavy meson molecules
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- Is molecule possible?
- Composite nature of states from data analysis
- QCD sum rules study of X(4350)
- wave bottomonia production from decay
- Charged bottomonium-like structures and
- Spin Partners of the resonances with a different approach than the Breit-Wigner parameterization
- Fully strange tetraquark states via QCD sum rules