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We study theoretically the feasibility to observe the $P_{css}$ with $I(J^P)=\\frac{1}{2}(\\frac{1}{2}^-)$ in the decays $\\Xi_b^0\\to \\eta \\eta_c \\Xi^0$ and $\\Omega_b^-\\to K^- \\eta_c \\Xi^0$. Indeed, within the model, the $\\eta_c \\Xi^0$ channel is the lowest mass pseudoscalar-baryon channel to which this pentaquark state couples, thus we can expect to observe its signal in the $\\eta_c \\Xi^0$ invariant mass distribution of the ment"},"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":"2406.16504","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-06-24T10:17:04Z","cross_cats_sorted":[],"title_canon_sha256":"bbf32ab8271901f44f196a4587da0adcd0606660d8b13cdfdeda2ea32382ab36","abstract_canon_sha256":"d784a5c974aef021ab2b21a292d983890f8ea3a0ee9d6dceec4c3bc024c7b7fc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:49:31.369600Z","signature_b64":"Y4owu7Dwn396zEM0mV5BrZdD1ve8wi/CZItLrfPb8aA+z0McJkbKHO1GSRSlgYOPpbk19TPo4kQWr9ozVljMCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c9d31cf139361c53da0d96bf2bb7f7f62a42ff136535e8aaa92939b10ba2dd3a","last_reissued_at":"2026-07-05T11:49:31.369151Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:49:31.369151Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Production of pentaquarks with hidden charm and double strangeness in $\\Xi_b$ and $\\Omega_b$ decays","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"E. 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Indeed, within the model, the $\\eta_c \\Xi^0$ channel is the lowest mass pseudoscalar-baryon channel to which this pentaquark state couples, thus we can expect to observe its signal in the $\\eta_c \\Xi^0$ invariant mass distribution of the ment"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.16504","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.16504/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2406.16504","created_at":"2026-07-05T11:49:31.369205+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.16504v1","created_at":"2026-07-05T11:49:31.369205+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.16504","created_at":"2026-07-05T11:49:31.369205+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZHJRZ4JZGYOF","created_at":"2026-07-05T11:49:31.369205+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZHJRZ4JZGYOFHWQN","created_at":"2026-07-05T11:49:31.369205+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZHJRZ4JZ","created_at":"2026-07-05T11:49:31.369205+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2603.11259","citing_title":"Comprehensive Mass Predictions: From Triply Heavy Baryons to Pentaquarks","ref_index":89,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04383","citing_title":"Production of $D_s\\bar{D}_s$ and $D\\bar{D}$ bound states in the $B$ decays within the Bethe-Salpeter framework","ref_index":33,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZHJRZ4JZGYOFHWQNS27SXN7X6Y","json":"https://pith.science/pith/ZHJRZ4JZGYOFHWQNS27SXN7X6Y.json","graph_json":"https://pith.science/api/pith-number/ZHJRZ4JZGYOFHWQNS27SXN7X6Y/graph.json","events_json":"https://pith.science/api/pith-number/ZHJRZ4JZGYOFHWQNS27SXN7X6Y/events.json","paper":"https://pith.science/paper/ZHJRZ4JZ"},"agent_actions":{"view_html":"https://pith.science/pith/ZHJRZ4JZGYOFHWQNS27SXN7X6Y","download_json":"https://pith.science/pith/ZHJRZ4JZGYOFHWQNS27SXN7X6Y.json","view_paper":"https://pith.science/paper/ZHJRZ4JZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.16504&json=true","fetch_graph":"https://pith.science/api/pith-number/ZHJRZ4JZGYOFHWQNS27SXN7X6Y/graph.json","fetch_events":"https://pith.science/api/pith-number/ZHJRZ4JZGYOFHWQNS27SXN7X6Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZHJRZ4JZGYOFHWQNS27SXN7X6Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZHJRZ4JZGYOFHWQNS27SXN7X6Y/action/storage_attestation","attest_author":"https://pith.science/pith/ZHJRZ4JZGYOFHWQNS27SXN7X6Y/action/author_attestation","sign_citation":"https://pith.science/pith/ZHJRZ4JZGYOFHWQNS27SXN7X6Y/action/citation_signature","submit_replication":"https://pith.science/pith/ZHJRZ4JZGYOFHWQNS27SXN7X6Y/action/replication_record"}},"created_at":"2026-07-05T11:49:31.369205+00:00","updated_at":"2026-07-05T11:49:31.369205+00:00"}