Observation of $\eta_{c}(2S) \to K^{+}K^{-}\eta$
BESIII Collaboration: M. Ablikim, M. N. Achasov, P. Adlarson, O., Afedulidis, X. C. Ai, R. Aliberti, A. Amoroso, Q. An, Y. Bai, O. Bakina, I., Balossino, Y. Ban, H.-R. Bao, V. Batozskaya, K. Begzsuren, N. Berger, M., Berlowski, M. Bertani, D. Bettoni, F. Bianchi, E. Bianco

TL;DR
This paper reports the first observation of the decay $ ext{eta}_c(2S) o K^+ K^- ext{eta}$ using a large sample of $ ext{psi}(3686)$ events, measuring its branching fraction and ratio to another decay mode, with significance over 6 sigma.
Contribution
First observation of $ ext{eta}_c(2S) o K^+ K^- ext{eta}$ decay and measurement of its branching fraction and ratio to $ ext{eta}_c(2S) o K^+ K^- ext{pi}^0$, providing new experimental data.
Findings
Decay $ ext{eta}_c(2S) o K^+ K^- ext{eta}$ observed with 6.2 sigma significance.
Branching fraction of $ ext{eta}_c(2S) o K^+ K^- ext{eta}$ measured as approximately 3.42 x 10^{-3}.
Ratio of branching fractions $ ext{eta}_c(2S) o K^+ K^- ext{eta}$ to $ ext{eta}_c(2S) o K^+ K^- ext{pi}^0$ is about 1.49.
Abstract
By analyzing events accumulated with the BESIII detector, the decay is observed for the first time with a significance of after considering systematic uncertainties. The product of the branching fractions of and is measured to be , where the first uncertainty is statistical, and the second one is systematic. The branching fraction of is determined to be , where the third uncertainty is due to the branching fraction of . Using a…
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Taxonomy
TopicsParticle physics theoretical and experimental studies · Black Holes and Theoretical Physics · Quantum Chromodynamics and Particle Interactions
