{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:2KDQNNJ2SH2FWZL53NQOGGA2Y5","short_pith_number":"pith:2KDQNNJ2","schema_version":"1.0","canonical_sha256":"d28706b53a91f45b657ddb60e3181ac74d47d88f48d9721059f86297b9d1013f","source":{"kind":"arxiv","id":"1107.0216","version":1},"attestation_state":"computed","paper":{"title":"Influence of tubular initial conditions on two-particle correlations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"F.Gardim, F.Grassi, R.P.G.Andrade, W.L.Qian, Y.Hama","submitted_at":"2011-07-01T13:04:17Z","abstract_excerpt":"A unified description of the near-side and away-side structures observed in two-particle correlations as function of delta eta-delta phi is proposed for low to moderate transverse momentum. It is based on the combined effect of tubular initial conditions and hydrodynamical expansion."},"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":"1107.0216","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-07-01T13:04:17Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"5d72a2894a2372e49dcf83d60eae5ef7191edffe3ff9dcdff72dfb70b24e3bc3","abstract_canon_sha256":"fc3466bdd865d4221e0080762f03748e0c4edc2c762765f20903cacc97e70be4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:25.900515Z","signature_b64":"X0wJ9WyrgRVpF+3ErrgZjvIsRXVMOmjguAiMaFqY4hHEjZYxNag+pZIMDLwmooIq3zsWiC9W3bxueKfTZP5FCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d28706b53a91f45b657ddb60e3181ac74d47d88f48d9721059f86297b9d1013f","last_reissued_at":"2026-05-18T02:01:25.899691Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:25.899691Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Influence of tubular initial conditions on two-particle correlations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"F.Gardim, F.Grassi, R.P.G.Andrade, W.L.Qian, Y.Hama","submitted_at":"2011-07-01T13:04:17Z","abstract_excerpt":"A unified description of the near-side and away-side structures observed in two-particle correlations as function of delta eta-delta phi is proposed for low to moderate transverse momentum. It is based on the combined effect of tubular initial conditions and hydrodynamical expansion."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.0216","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":""},"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":"1107.0216","created_at":"2026-05-18T02:01:25.899834+00:00"},{"alias_kind":"arxiv_version","alias_value":"1107.0216v1","created_at":"2026-05-18T02:01:25.899834+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.0216","created_at":"2026-05-18T02:01:25.899834+00:00"},{"alias_kind":"pith_short_12","alias_value":"2KDQNNJ2SH2F","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_16","alias_value":"2KDQNNJ2SH2FWZL5","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_8","alias_value":"2KDQNNJ2","created_at":"2026-05-18T12:26:18.847500+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/2KDQNNJ2SH2FWZL53NQOGGA2Y5","json":"https://pith.science/pith/2KDQNNJ2SH2FWZL53NQOGGA2Y5.json","graph_json":"https://pith.science/api/pith-number/2KDQNNJ2SH2FWZL53NQOGGA2Y5/graph.json","events_json":"https://pith.science/api/pith-number/2KDQNNJ2SH2FWZL53NQOGGA2Y5/events.json","paper":"https://pith.science/paper/2KDQNNJ2"},"agent_actions":{"view_html":"https://pith.science/pith/2KDQNNJ2SH2FWZL53NQOGGA2Y5","download_json":"https://pith.science/pith/2KDQNNJ2SH2FWZL53NQOGGA2Y5.json","view_paper":"https://pith.science/paper/2KDQNNJ2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1107.0216&json=true","fetch_graph":"https://pith.science/api/pith-number/2KDQNNJ2SH2FWZL53NQOGGA2Y5/graph.json","fetch_events":"https://pith.science/api/pith-number/2KDQNNJ2SH2FWZL53NQOGGA2Y5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2KDQNNJ2SH2FWZL53NQOGGA2Y5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2KDQNNJ2SH2FWZL53NQOGGA2Y5/action/storage_attestation","attest_author":"https://pith.science/pith/2KDQNNJ2SH2FWZL53NQOGGA2Y5/action/author_attestation","sign_citation":"https://pith.science/pith/2KDQNNJ2SH2FWZL53NQOGGA2Y5/action/citation_signature","submit_replication":"https://pith.science/pith/2KDQNNJ2SH2FWZL53NQOGGA2Y5/action/replication_record"}},"created_at":"2026-05-18T02:01:25.899834+00:00","updated_at":"2026-05-18T02:01:25.899834+00:00"}