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In the present work, we investigate the production of $P_{c}$ and $Z_c(3900)/Z_{cs}(3985)$ states in the processes of $pi p rightarrow Z_{c}(3900) P_{c} $/$Kprightarrow Z_{cs}(3985) P_{c}$ with an effective Lagrangian approach. Our estimations indicates that the cross sections depends on the model parameters and beam energies, in particular, the cross sections for $pi p to Z_c(3900) P_c(4312)$ and $pi p to Z_c(3900) P_c(4440)$ are similar and can reach up to 10 nb, while those for $pi p to Z_c(3900) P_c(4457)$ can be 30 nb. As for $Kp to Z_{cs}(3985)P_c$, the cross sections are about 2.5 times smaller than those for $pi p to Z_c(3900) P_c$. The discussed processes in the present work, especially $pi p to Z_c(3900) P_c(4457)$, may be accessible by the the high-energy pion and kaon beams in the facilities of J-PARC and COMPASS.
We investigate the reaction $pi^- p to pi^- J/psi p$ via the open-charm hadron rescattering diagrams. Due to the presence of the triangle singularity (TS) in the rescattering amplitudes, the TS peaks can simulate the pentaquark-like resonances arisin
Many charmonium-like and bottomonium-like $XYZ$ resonances have been observed by the Belle, Babar, CLEO and BESIII collaborations in the past decade. They are difficult to fit in the conventional quark model and thus are considered as candidates of e
Some of the recent progress in the physics of pion production induced by neutrinos on nucleons and nuclei is reviewed from a theoretical perspective. The importance of Watsons theorem to reconcile ANL and BNL data with the off-diagonal Goldberger-Tre
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There are two mass generating mechanisms in the standard model of particle physics (SM). One is related to the Higgs boson and fairly well understood. The other is embedded in quantum chromodynamics (QCD), the SMs strong interaction piece; and althou