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Adopting the one-boson-exchange model and including the coupled-channel effects, we derive the effective potentials for all allowed quantum numbers $I(J^P) = 1/2(1/2^+)$, $1/2(3/2^+)$, $1/2(5/2^+)$, $1/2(7/2^+)$, $3/2(1/2^+)$, $3/2(3/2^+)$, $3/2(5/2^+)$, and $3/2(7/2^+)$. We then solve t"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2607.14913","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-16T12:32:40Z","cross_cats_sorted":[],"title_canon_sha256":"06922a55b0b2d31dec947a57404ccbc55b2ee3705deaf2e2c302fae9683d43ee","abstract_canon_sha256":"2bf24aa9faa85817b018332dc90662bff547df15471c845aad5d3cf2115c7c3a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-17T01:21:58.483021Z","signature_b64":"8C1ORkQ7hsp1RGhLtuG4FCrMhMDeuvnAl2XDhmlxuYRaAr9shuwQjBFDaup9EVLjjhMHkaJYHyeY3O7UAUOWCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c16a817588e611f2d82e52b721155b4d156c244a6ce1779550d3fb978cd534cb","last_reissued_at":"2026-07-17T01:21:58.482172Z","signature_status":"signed_v1","first_computed_at":"2026-07-17T01:21:58.482172Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Possible hidden-bottom molecular pentaquarks from $P$-wave $\\Lambda_bB^{(*)}/\\Sigma_b^{(*)}B^{(*)}$ interactions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fu-Lai Wang, Qi Huang, Rui Chen, Yu-Xin Wan","submitted_at":"2026-07-16T12:32:40Z","abstract_excerpt":"In this work, we perform a systematic investigation of the hidden-bottom molecular pentaquark states, encompassing both bound states and resonances, which originate from the $P$-wave interactions between ground-state bottom baryons ($\\Lambda_b$, $\\Sigma_b^{(*)}$) and ground-state antibottom mesons ($B^{(*)}$). Adopting the one-boson-exchange model and including the coupled-channel effects, we derive the effective potentials for all allowed quantum numbers $I(J^P) = 1/2(1/2^+)$, $1/2(3/2^+)$, $1/2(5/2^+)$, $1/2(7/2^+)$, $3/2(1/2^+)$, $3/2(3/2^+)$, $3/2(5/2^+)$, and $3/2(7/2^+)$. 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