Probing hidden-charm pentaquarks from the $πN\rightarrow J/ψN$ reaction
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arXiv
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| Autori principali: | , , , |
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| Natura: | Preprint |
| Pubblicazione: |
2026
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| _version_ | 1866917540272275456 |
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| author | Clymton, Samson Ryu, Sun-Young Ahn, Jung-Keun Kim, Hyun-Chul |
| author_facet | Clymton, Samson Ryu, Sun-Young Ahn, Jung-Keun Kim, Hyun-Chul |
| contents | We investigate the dynamical generation of hidden-charm pentaquark resonances in the $πN \to J/ψN$ reaction utilizing an off-shell coupled-channel formalism. Motivated by the absence of pentaquark signals in $J/ψ$ photoproduction, we evaluate rescattering effects with two-body kernel amplitudes constructed from effective Lagrangians that explicitly incorporate $t$-channel meson and $u$-channel baryon exchanges. We demonstrate that the $u$-channel $Λ_c$ exchange, of which an analogous contribution is absent in the photoproduction kernel, greatly enhances the rescattering contributions through the $\bar{D}^{(*)}Σ_c$ intermediate states. Consequently, the $\bar{D}^{(*)}Σ_c^{(*)}$ channels yield contributions of comparable magnitude to the $\bar{D}^{(*)}Λ_c$ channels, directly leading to prominent pentaquark signals. The partial-wave analysis reveals that the $P_{c\bar{c}}(4312)$ and $P_{c\bar{c}}(4457)$ states emerge as clear peak structures with $J^P=1/2^-$ and $3/2^-$, respectively. In contrast, the $P_{c\bar{c}}(4380)$ and $J^P=5/2^-$ states are strongly suppressed because the $Λ_c$ exchange does not provide the required tensor interactions. The result for the total cross section reaches the microbarn level at the peak positions. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2605_28285 |
| institution | arXiv |
| publishDate | 2026 |
| record_format | arxiv |
| spellingShingle | Probing hidden-charm pentaquarks from the $πN\rightarrow J/ψN$ reaction Clymton, Samson Ryu, Sun-Young Ahn, Jung-Keun Kim, Hyun-Chul High Energy Physics - Phenomenology High Energy Physics - Experiment We investigate the dynamical generation of hidden-charm pentaquark resonances in the $πN \to J/ψN$ reaction utilizing an off-shell coupled-channel formalism. Motivated by the absence of pentaquark signals in $J/ψ$ photoproduction, we evaluate rescattering effects with two-body kernel amplitudes constructed from effective Lagrangians that explicitly incorporate $t$-channel meson and $u$-channel baryon exchanges. We demonstrate that the $u$-channel $Λ_c$ exchange, of which an analogous contribution is absent in the photoproduction kernel, greatly enhances the rescattering contributions through the $\bar{D}^{(*)}Σ_c$ intermediate states. Consequently, the $\bar{D}^{(*)}Σ_c^{(*)}$ channels yield contributions of comparable magnitude to the $\bar{D}^{(*)}Λ_c$ channels, directly leading to prominent pentaquark signals. The partial-wave analysis reveals that the $P_{c\bar{c}}(4312)$ and $P_{c\bar{c}}(4457)$ states emerge as clear peak structures with $J^P=1/2^-$ and $3/2^-$, respectively. In contrast, the $P_{c\bar{c}}(4380)$ and $J^P=5/2^-$ states are strongly suppressed because the $Λ_c$ exchange does not provide the required tensor interactions. The result for the total cross section reaches the microbarn level at the peak positions. |
| title | Probing hidden-charm pentaquarks from the $πN\rightarrow J/ψN$ reaction |
| topic | High Energy Physics - Phenomenology High Energy Physics - Experiment |
| url | https://arxiv.org/abs/2605.28285 |