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Observation of charmonium hc radiative decays to multiple light hadrons and the tensor state f2 (1270)

2025-06-18 Author:
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The BESIII Collaboration recently reported “Observation of charmonium hc radiative decays to multiple light hadrons and the tensor state f2 (1270)”. The paper has been published online in Physical Review Letter on June. 17, 2025. [Phys. Rev. Lett. 134, 241902 (2025)].
The study of charmonium radiative decay provides a unique opportunity to deepen our understanding of quantum chromodynamics (QCD) by testing theoretical predictions with experimental observations. Unlike J/ψ and ψ(3686), the study of the radiative decay of the P-wave singlet hc charmonium state to light hadrons is limited. Besides the radiative transition  hc→γηc, only two radiative decays hc→γη and hc →γη' have been observed. The experimental results of hc radiative decays were significantly different from the theoretical predicted value 5.5% of B(hc→γ+2g).
Using a data sample of (27.12±0.14)×108 ψ(3686) events collected by the BESIII detector, four modes of hc radiative decays to multiple light hadrons are observed via ψ(3686)→π0 hc for the first time. The clear signal of hc→γX (X=π+ π-, π+ π- η, 2(π+ π-), ppbar) are shown in Fig.1 with significance larger than 5σ.  The corresponding branching fractions are precisely measured. The sum of known branching fractions of the hc radiative decay including the results of this analysis is approximately 0.8%, which is still significantly lower than the theoretical prediction. This discrepancy highlights the need for further exploration of hc radiative decays. Moreover, hc radiative decay to f2(1270) is observed with a significance of 5.1σ. This is the first observation of hc radiative decay to a tensor state. The branching fraction of hc→γf2(1270)→γπ+ π- is an order of magnitude smaller than that in J/ψ decay. This measurement could be employed to investigate the quark and glueball mixing parameters of f2(1270). These findings significantly advance our understanding of charmonium decay mechanisms and provides a promising path towards searching for exotic states.

Figure 1: Fits to the M(γX) invariant mass distributions, whereXrepresents π+ π-, π+ π- η, 2(π+ π-),  and ppbar, respectively.

URL: https://journals.aps.org/prl/abstract/10.1103/v4hf-s8x8
DOI: https://doi.org/10.1103/v4hf-s8x8