{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:CRFAIVUFSWWWL5AOM45V4HSJIA","short_pith_number":"pith:CRFAIVUF","schema_version":"1.0","canonical_sha256":"144a04568595ad65f40e673b5e1e49400100e6d1c42397638cab2b6bef55ac50","source":{"kind":"arxiv","id":"nucl-ex/0409021","version":1},"attestation_state":"computed","paper":{"title":"Scaling of Charged Particle Production in d+Au Collisions at sqrt(s_NN) = 200 GeV","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"et al, the PHOBOS Collaboration: B.B. Back","submitted_at":"2004-09-24T22:58:30Z","abstract_excerpt":"The measured pseudorapidity distributions of primary charged particles over a wide pseudorapidity range of |eta| < 5.4 and integrated charged particle multiplicities in d+Au collisions at sqrt(s_NN) = 200 GeV are presented as a function of collision centrality. The longitudinal features of d+Au collisions at sqrt(s_NN) = 200 GeV are found to be very similar to those seen in p + A collisions at lower energies. The total multiplicity of charged particles is found to scale with the total number of participants according to N^{dAu}_{ch} = 1/2 <N_{part}> N^{pp}_{ch} and the energy dependence of the"},"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":"nucl-ex/0409021","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-ex","submitted_at":"2004-09-24T22:58:30Z","cross_cats_sorted":[],"title_canon_sha256":"c499cefbe76927f887905e8a7d7db9079ab141f8dcd000b5a6dce9afee52cf70","abstract_canon_sha256":"12b1683b4d3de63a2bb564693adb19f70a7878aa505a3dc14c0a919d53098874"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:20:35.087469Z","signature_b64":"lwaoPszD4hT/kEQIoYif7VhtcX6SFNHtYYn8I1WSu/TS9ijdpVZt4mXxD5v9PhtezJO6+MP2h5Q7eryCWArCAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"144a04568595ad65f40e673b5e1e49400100e6d1c42397638cab2b6bef55ac50","last_reissued_at":"2026-07-04T15:20:35.086932Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:20:35.086932Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scaling of Charged Particle Production in d+Au Collisions at sqrt(s_NN) = 200 GeV","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"et al, the PHOBOS Collaboration: B.B. Back","submitted_at":"2004-09-24T22:58:30Z","abstract_excerpt":"The measured pseudorapidity distributions of primary charged particles over a wide pseudorapidity range of |eta| < 5.4 and integrated charged particle multiplicities in d+Au collisions at sqrt(s_NN) = 200 GeV are presented as a function of collision centrality. The longitudinal features of d+Au collisions at sqrt(s_NN) = 200 GeV are found to be very similar to those seen in p + A collisions at lower energies. The total multiplicity of charged particles is found to scale with the total number of participants according to N^{dAu}_{ch} = 1/2 <N_{part}> N^{pp}_{ch} and the energy dependence of the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0409021","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/nucl-ex/0409021/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":"nucl-ex/0409021","created_at":"2026-07-04T15:20:35.087001+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-ex/0409021v1","created_at":"2026-07-04T15:20:35.087001+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-ex/0409021","created_at":"2026-07-04T15:20:35.087001+00:00"},{"alias_kind":"pith_short_12","alias_value":"CRFAIVUFSWWW","created_at":"2026-07-04T15:20:35.087001+00:00"},{"alias_kind":"pith_short_16","alias_value":"CRFAIVUFSWWWL5AO","created_at":"2026-07-04T15:20:35.087001+00:00"},{"alias_kind":"pith_short_8","alias_value":"CRFAIVUF","created_at":"2026-07-04T15:20:35.087001+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/CRFAIVUFSWWWL5AOM45V4HSJIA","json":"https://pith.science/pith/CRFAIVUFSWWWL5AOM45V4HSJIA.json","graph_json":"https://pith.science/api/pith-number/CRFAIVUFSWWWL5AOM45V4HSJIA/graph.json","events_json":"https://pith.science/api/pith-number/CRFAIVUFSWWWL5AOM45V4HSJIA/events.json","paper":"https://pith.science/paper/CRFAIVUF"},"agent_actions":{"view_html":"https://pith.science/pith/CRFAIVUFSWWWL5AOM45V4HSJIA","download_json":"https://pith.science/pith/CRFAIVUFSWWWL5AOM45V4HSJIA.json","view_paper":"https://pith.science/paper/CRFAIVUF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-ex/0409021&json=true","fetch_graph":"https://pith.science/api/pith-number/CRFAIVUFSWWWL5AOM45V4HSJIA/graph.json","fetch_events":"https://pith.science/api/pith-number/CRFAIVUFSWWWL5AOM45V4HSJIA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CRFAIVUFSWWWL5AOM45V4HSJIA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CRFAIVUFSWWWL5AOM45V4HSJIA/action/storage_attestation","attest_author":"https://pith.science/pith/CRFAIVUFSWWWL5AOM45V4HSJIA/action/author_attestation","sign_citation":"https://pith.science/pith/CRFAIVUFSWWWL5AOM45V4HSJIA/action/citation_signature","submit_replication":"https://pith.science/pith/CRFAIVUFSWWWL5AOM45V4HSJIA/action/replication_record"}},"created_at":"2026-07-04T15:20:35.087001+00:00","updated_at":"2026-07-04T15:20:35.087001+00:00"}