3,127 research outputs found

    Analysis of the Pc(4380)P_c(4380) and Pc(4450)P_c(4450) as pentaquark states in the diquark model with QCD sum rules

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    In this article, we construct the diquark-diquark-antiquark type interpolating currents, and study the masses and pole residues of the JP=32βˆ’J^P={\frac{3}{2}}^- and 52+{\frac{5}{2}}^+ hidden-charmed pentaquark states in details with the QCD sum rules by calculating the contributions of the vacuum condensates up to dimension-10 in the operator product expansion. In calculations, we use the formula ΞΌ=MPc2βˆ’(2Mc)2\mu=\sqrt{M^2_{P_c}-(2{\mathbb{M}}_c)^2} to determine the energy scales of the QCD spectral densities. The present predictions favor assigning the Pc(4380)P_c(4380) and Pc(4450)P_c(4450) to be the 32βˆ’{\frac{3}{2}}^- and 52+{\frac{5}{2}}^+ pentaquark states, respectively.Comment: 18 pages, 5 figure

    Strong decay of the heavy tensor mesons with QCD sum rules

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    In the article, we calculate the hadronic coupling constants GD2βˆ—DΟ€G_{D_2^*D\pi}, GDs2βˆ—DKG_{D_{s2}^*DK}, GB2βˆ—BΟ€G_{B_2^*B\pi}, GBs2βˆ—BKG_{B_{s2}^*BK} with the three-point QCD sum rules, then study the two body strong decays D2βˆ—(2460)β†’DΟ€D_2^*(2460)\to D\pi, Ds2βˆ—(2573)β†’DKD_{s2}^*(2573)\to DK, B2βˆ—(5741)β†’BΟ€B_2^*(5741)\to B\pi, Bs2βˆ—(5840)β†’BKB_{s2}^*(5840)\to BK, and make predictions to be confronted with the experimental data in the future.Comment: 12 pages, 2 figure

    Lowest vector tetraquark states: Y(4260/4220)Y(4260/4220) or Zc(4100)Z_c(4100)

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    In this article, we take the Y(4260/4220)Y(4260/4220) as the vector tetraquark state with JPC=1βˆ’βˆ’J^{PC}=1^{--}, and construct the CΞ³5βŠ—βˆ‚β†”ΞΌβŠ—Ξ³5CC\gamma_5\otimes\stackrel{\leftrightarrow}{\partial}_\mu\otimes \gamma_5C type diquark-antidiquark current to study its mass and pole residue with the QCD sum rules in details by taking into account the vacuum condensates up to dimension 10 in a consistent way. The predicted mass MY=4.24Β±0.10 GeVM_{Y}=4.24\pm0.10\,\rm{GeV} is in excellent agreement with experimental data and supports assigning the Y(4260/4220)Y(4260/4220) to be the CΞ³5βŠ—βˆ‚β†”ΞΌβŠ—Ξ³5CC\gamma_5\otimes\stackrel{\leftrightarrow}{\partial}_\mu\otimes \gamma_5C type vector tetraquark state, and disfavors assigning the Zc(4100)Z_c(4100) to be the CΞ³5βŠ—βˆ‚β†”ΞΌβŠ—Ξ³5CC\gamma_5\otimes\stackrel{\leftrightarrow}{\partial}_\mu\otimes \gamma_5C type vector tetraquark state. It is the first time that the QCD sum rules have reproduced the mass of the Y(4260/4220)Y(4260/4220) as a vector tetraquark state.Comment: 13 pages, 4 figures. arXiv admin note: text overlap with arXiv:1803.0574
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