{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:5VNZAFM2KGOA6KSXCDNFDBSOXI","short_pith_number":"pith:5VNZAFM2","schema_version":"1.0","canonical_sha256":"ed5b90159a519c0f2a5710da51864eba144fe5e789253d5b2e6b338660ae962f","source":{"kind":"arxiv","id":"1107.0209","version":2},"attestation_state":"computed","paper":{"title":"rho-rho-N and rho-rho-Delta molecules with $J^P=5/2^{+}$ and $J^P=7/2^{+}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Bao-Xi Sun, E. Oset, Hua-Xing Chen","submitted_at":"2011-07-01T12:27:00Z","abstract_excerpt":"The rho-rho-N and rho-rho-Delta three-body systems have been studied within the framework of the fixed center approximation of Faddeev equation. The rho-rho interaction in isospin I=0, spin S=2 is strongly attractive, and so are the N-rho, Delta-rho interactions. This leads to bound states of both rho-rho-N and rho-rho-Delta. We find peaks of the modulus squared of the scattering matrix around 2227 MeV for rho-rho-N, and 2372 MeV for rho-rho-Delta. Yet, the strength of the peak for the rho-rho-N amplitude is much smaller than for rho-rho-Delta, weakening the case for a rho-rho-N bound state, o"},"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":"1107.0209","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-07-01T12:27:00Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"dd5c56199ad0a9abe3f54d0b71f93519037b105aa23c849b0ffad5c9dd22131c","abstract_canon_sha256":"ea84985429c4d2a798c1296799fe7962ae043a060df4cfbd15a176fb1e7c02ae"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:25.934829Z","signature_b64":"m3na8mDTNcq2asTj1TmWCDZM80kXcr9VcL3juwAIIn2kXQVjczRMakkARFNutGJnH9Jw/DVxWbdynNx3PSmZBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ed5b90159a519c0f2a5710da51864eba144fe5e789253d5b2e6b338660ae962f","last_reissued_at":"2026-05-18T02:01:25.934205Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:25.934205Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"rho-rho-N and rho-rho-Delta molecules with $J^P=5/2^{+}$ and $J^P=7/2^{+}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Bao-Xi Sun, E. Oset, Hua-Xing Chen","submitted_at":"2011-07-01T12:27:00Z","abstract_excerpt":"The rho-rho-N and rho-rho-Delta three-body systems have been studied within the framework of the fixed center approximation of Faddeev equation. The rho-rho interaction in isospin I=0, spin S=2 is strongly attractive, and so are the N-rho, Delta-rho interactions. This leads to bound states of both rho-rho-N and rho-rho-Delta. We find peaks of the modulus squared of the scattering matrix around 2227 MeV for rho-rho-N, and 2372 MeV for rho-rho-Delta. Yet, the strength of the peak for the rho-rho-N amplitude is much smaller than for rho-rho-Delta, weakening the case for a rho-rho-N bound state, o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.0209","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1107.0209","created_at":"2026-05-18T02:01:25.934298+00:00"},{"alias_kind":"arxiv_version","alias_value":"1107.0209v2","created_at":"2026-05-18T02:01:25.934298+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.0209","created_at":"2026-05-18T02:01:25.934298+00:00"},{"alias_kind":"pith_short_12","alias_value":"5VNZAFM2KGOA","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_16","alias_value":"5VNZAFM2KGOA6KSX","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_8","alias_value":"5VNZAFM2","created_at":"2026-05-18T12:26:20.644004+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5VNZAFM2KGOA6KSXCDNFDBSOXI","json":"https://pith.science/pith/5VNZAFM2KGOA6KSXCDNFDBSOXI.json","graph_json":"https://pith.science/api/pith-number/5VNZAFM2KGOA6KSXCDNFDBSOXI/graph.json","events_json":"https://pith.science/api/pith-number/5VNZAFM2KGOA6KSXCDNFDBSOXI/events.json","paper":"https://pith.science/paper/5VNZAFM2"},"agent_actions":{"view_html":"https://pith.science/pith/5VNZAFM2KGOA6KSXCDNFDBSOXI","download_json":"https://pith.science/pith/5VNZAFM2KGOA6KSXCDNFDBSOXI.json","view_paper":"https://pith.science/paper/5VNZAFM2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1107.0209&json=true","fetch_graph":"https://pith.science/api/pith-number/5VNZAFM2KGOA6KSXCDNFDBSOXI/graph.json","fetch_events":"https://pith.science/api/pith-number/5VNZAFM2KGOA6KSXCDNFDBSOXI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5VNZAFM2KGOA6KSXCDNFDBSOXI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5VNZAFM2KGOA6KSXCDNFDBSOXI/action/storage_attestation","attest_author":"https://pith.science/pith/5VNZAFM2KGOA6KSXCDNFDBSOXI/action/author_attestation","sign_citation":"https://pith.science/pith/5VNZAFM2KGOA6KSXCDNFDBSOXI/action/citation_signature","submit_replication":"https://pith.science/pith/5VNZAFM2KGOA6KSXCDNFDBSOXI/action/replication_record"}},"created_at":"2026-05-18T02:01:25.934298+00:00","updated_at":"2026-05-18T02:01:25.934298+00:00"}