Revisit the X(4274)X(4274) as the axialvector tetraquark state

preprint2019arXivOpen access

Abstract

In this article, we construct the [sc]A[sˉcˉ]V−[sc]V[sˉcˉ]A[sc]_A[\bar{s}\bar{c}]_V-[sc]_V[\bar{s}\bar{c}]_A type tensor current to study the mass and width of the X(4274)X(4274) with the QCD sum rules in details. The predicted mass MX=(4.27±0.09) GeVM_{X}=(4.27\pm0.09) \, \rm{GeV} for the JPC=1++J^{PC}=1^{++} tetraquark state is in excellent agreement with the experimental data $4273.3 \pm 8.3 ^{+17.2}_{-3.6} \mbox MeV}$ from the LHCb collaboration. The central value of the width Γ(X(4274)→J/ψϕ)=47.9 MeVΓ(X(4274)\to J/ψϕ)=47.9\,{\rm{MeV}} is in excellent agreement with the experimental data $56 \pm 11 ^{+8}_{-11} \mbox MeV}}$ from the LHCb collaboration. The present work supports assigning the X(4274)X(4274) to be the JPC=1++J^{PC}=1^{++} [sc]A[sˉcˉ]V−[sc]V[sˉcˉ]A[sc]_A[\bar{s}\bar{c}]_V-[sc]_V[\bar{s}\bar{c}]_A tetraquark state with a relative P-wave between the diquark and antidiquark constituents. Furthermore, we obtain the mass of the [sc]A[sˉcˉ]V−[sc]V[sˉcˉ]A[sc]_A[\bar{s}\bar{c}]_V-[sc]_V[\bar{s}\bar{c}]_A type tetraquark state with JPC=1−+J^{PC}=1^{-+} as a byproduct.

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