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In our discussion, while the main contribution to $\\Lambda_b\\to K^-J/\\psi p$ is from the non-perturbative process via the doubly charmful $b\\to c\\bar cs$ transition, we propose that the $\\Lambda_b\\to {\\cal P}_{c1,c2}\\to J/\\psi p$ transitions are partly contribute to the $\\Lambda_b\\to K^-({\\cal P}_{c1,c2}\\to)J/\\psi p$ decays, in which the required $c\\bar c$ pair is formed by th"},"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":"1706.02460","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-06-08T07:17:59Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"6c8b6d31af45b2a9f694504126962226406ade769f0f9e4e5ea1a25f65ca4548","abstract_canon_sha256":"dae320f81a53c65e098e3946e30919409ecde4fb39e61bcacd5e7d2acaaee7ec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:42:45.409441Z","signature_b64":"T8d4sM+sgdrK6w0MXGb39R74YMaM+r/dMcixyQ9LiBZV5OHGVRci32XU8kcniuUCiwgQHkYD6u3qcrQC6v76Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e8277cfb618c351bf412776d8411023e7194ce86dc1ad690bd96dbf9f66f5f2f","last_reissued_at":"2026-05-18T00:42:45.408891Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:42:45.408891Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pentaquarks in semileptonic $\\Lambda_b$ decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"C.Q. 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