Abstract
Within the effective Lagrangian approach, we study the $p\bar{p} \rightarrow \psi\eta$ [$\psi\equiv\psi(3686)$, $J/\psi$] reaction at the low energy where the contributions from nucleon pole and low-lying nucleon resonances, $N(1520)$, $N(1535)$ and $N(1650)$ are considered. All the model parameters are determined with the help of current experimental data on the decay of $\psi \to p \bar{p} \eta$. Within the model parameters, the total and differential cross sections of the $p\bar{p} \rightarrow \psi\eta$ reaction are predicted. We show that the relative phases between different amplitudes of different nucleon resonance will change significantly the angular distributions of the $\bar{p} p \to \psi \eta$ reaction. Therefore, we conclude that these reactions are suitable to study experimentally the properties of the low-lying nucleon resonance and the reaction mechanisms. We hope that these theoretical calculations can be tested by future experiments.
Highlights
The charmonium, Hc, production in the pp → HcX reaction is an interesting tool to gain a deeper understanding of the strong interaction and of the nature of the hadrons [1]
We show that the relative phases between different amplitudes of different nucleon resonance will change significantly the angular distributions of the pp → ψη reaction
The forthcoming Proton Annihilations at Darmstadt (P ANDA) will be an ideal platform to carry out the study of hadron physics
Summary
The charmonium, Hc, production in the pp → HcX (the X is a light meson) reaction is an interesting tool to gain a deeper understanding of the strong interaction and of the nature of the hadrons [1]. Lin, Xu, and Liu [7] considered the contributions of the intermediate nucleon pole and the effect of form factors (FFs) on charmonium production in. Since the experimental data on the ψ → pp X decays become rich, we can consider the contributions from nucleon resonances in the pp → ψX reaction, where parameters can be fixed through the process of ψ → pp X. In this work, we will calculate the production cross sections of the process pp → ψη within the effective Lagrangian approach and give the angular distributions, where the contributions from the nucleon pole and three NÃ states are considered.
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