Decays of Dsj*(2317) and Dsj(2460) Mesons in the Quark Model

  • We study the decay widths of the narrow resonances D sj *(2317) and D sj(2460) in the chiral quark model, together with the well-known D *and D s *mesons. All the parameters in our calculation are taken from Godfrey and Isgur's quark model except the π 0-η mixing angle which is fixed by the D s *decay widths. The calculated electromagnetic decay widths agree with those from other groups and the experimental data available quite well. However, the pionic decay widths of D sj(2317) and D sj(2460) are too small to fit the experimental data. We suspect that the simple chiral quark pion axial-vector interaction Hamiltonian is not suitable for hadron strong decays of D sj(2317) and D sj(2460).
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WANG Feng-Lin, CHEN Xiao-Lin, LU Da-Hai, ZHU Shi-Lin and DENG Wei-Zhen. Decays of D sj *(2317) and D sj(2460) Mesons in the Quark Model[J]. Chinese Physics C, 2006, 30(11): 1041-1047.
WANG Feng-Lin, CHEN Xiao-Lin, LU Da-Hai, ZHU Shi-Lin and DENG Wei-Zhen. Decays of D sj *(2317) and D sj(2460) Mesons in the Quark Model[J]. Chinese Physics C, 2006, 30(11): 1041-1047. shu
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Received: 2006-04-13
Revised: 2006-05-11
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    Decays of Dsj*(2317) and Dsj(2460) Mesons in the Quark Model

      Corresponding author:DENG Wei-Zhen,
    • Department of Physics, Peking University, Beijing 100871, China

      Abstract:We study the decay widths of the narrow resonances Dsj*(2317) and Dsj(2460) in the chiral quark model, together with the well-known D*and Ds*mesons. All the parameters in our calculation are taken from Godfrey and Isgur's quark model except the π0-η mixing angle which is fixed by the Ds*decay widths. The calculated electromagnetic decay widths agree with those from other groups and the experimental data available quite well. However, the pionic decay widths of Dsj(2317) and Dsj(2460) are too small to fit the experimental data. We suspect that the simple chiral quark pion axial-vector interaction Hamiltonian is not suitable for hadron strong decays of Dsj(2317) and Dsj(2460).

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