Abstract
In this paper, the dilepton electromagnetic decays χcJ(1 P) → J/ ψe+e- and χcJ(1 P) → Jψμ+μ-, where χcJ denotes χc, χc 1 and χc 2, are calculated systematically in the improved Bethe–Salpeter method. The numerical results of decay widths and the invariant mass distributions of the final lepton pairs are given. The comparison is made with the recently measured experimental data of BESIII. It is shown that for the cases including e+e-, the gauge invariance is decisive and should be considered carefully. For the processes of χcJ(1 P) → J/ ψe+e-, the branching fraction are: B[χc0(1P)→J/ψe+e-]=1.06-0.18+0.16×10-4, B[χc1(1P)→J/ψe+e-]=2.88-0.53+0.50×10-3, and B[χc2(1P)→J/ψe+e-]=1.74-0.21+0.22×10-3. The calculated branching fractions of χcJ(1 P) → J/ ψμ+μ- channels are: B[χc0(1P)→J/ψμ+μ-]=3.80-0.64+0.59×10-6, B[χc1(1P)→J/ψμ+μ-]=2.04-0.38+0.36×10-4, and B[χc2(1P)→J/ψμ+μ-]=1.66-0.19+0.19×10-4.
| Original language | English |
|---|---|
| Article number | 997 |
| Journal | European Physical Journal C |
| Volume | 79 |
| Issue number | 12 |
| DOIs | |
| State | Published - 1 Dec 2019 |
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