Abstract
The radiative decays χc1(3872) → ψ(2S) γ and χc1(3872) → J/ψγ are used to probe the nature of the χc1(3872) state using proton-proton collision data collected with the LHCb detector, corresponding to an integrated luminosity of 9 fb−1. Using the B+ → χc1(3872)K+ decay, the χc1(3872) → ψ(2S) γ process is observed for the first time and the ratio of its partial width to that of the χc1(3872) → J/ψγ decay is measured to be
Γχc1(3872)→ψ(2S)γ/Γχc1(3872)→J/ψγ= 1.67 ± 0.21 ± 0.12 ± 0.04,
where the first uncertainty is statistical, the second systematic and the third is due to the uncertainties on the branching fractions of the ψ(2S) and J/ψ mesons. The measured ratio makes the interpretation of the χc1(3872) state as a pure D0
D̅∗0 + D̅ 0 D*0 molecule questionable and strongly indicates a sizeable compact charmonium or tetraquark component within the χc1(3872) state.| Original language | English |
|---|---|
| Article number | 121 |
| Number of pages | 31 |
| Journal | Journal of High Energy Physics |
| Volume | 2024 |
| Issue number | 11 |
| DOIs | |
| Publication status | Published - 21 Nov 2024 |
Bibliographical note
Publisher Copyright:© The Author(s) 2024.
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