{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:7HPWOJB264BLBT6KZVAUGHD6H7","short_pith_number":"pith:7HPWOJB2","schema_version":"1.0","canonical_sha256":"f9df67243af702b0cfcacd41431c7e3fe338df030f5d00f4bbe47a3982f2b1b9","source":{"kind":"arxiv","id":"nucl-ex/0606014","version":1},"attestation_state":"computed","paper":{"title":"Scaling Properties of Hyperon Production in Au+Au Collisions at sqrt(s_NN) = 200 GeV","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"et al, J.Adams, STAR Collaboration","submitted_at":"2006-06-07T12:16:59Z","abstract_excerpt":"We present the scaling properties of Lambda, Xi, Omega and their anti-particles produced at mid-rapidity in Au+Au collisions at RHIC at sqrt(s_NN) = 200 GeV. The yield of multi-strange baryons per participant nucleon increases from peripheral to central collisions more rapidly than the Lambda yield, which appears to correspond to an increasing strange quark density of matter produced. The value of the strange phase space occupancy factor gamma_s, obtained from a thermal model fit to the data, approaches unity for the most central collisions. We also show that the nuclear modification factors, "},"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/0606014","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-ex","submitted_at":"2006-06-07T12:16:59Z","cross_cats_sorted":[],"title_canon_sha256":"d4ee0b92de528bf44bdbceb1a9f3c10bf68f28b3d6987040ad41002bb9e3d642","abstract_canon_sha256":"83e9aa06429c9f2a07245d9c0aa176e63213f130c2321411de071a5b6d1d4c87"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:26:11.126388Z","signature_b64":"uPPmoRHjcW1W3H+MJyPWrFIL/uhIF9I6RcEdvwwQr3zwYWSZZ9rO/jT0NzlEgupdg9/OMd6i4b7Uw5JnqtzRDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f9df67243af702b0cfcacd41431c7e3fe338df030f5d00f4bbe47a3982f2b1b9","last_reissued_at":"2026-07-04T15:26:11.125975Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:26:11.125975Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scaling Properties of Hyperon Production in Au+Au Collisions at sqrt(s_NN) = 200 GeV","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"et al, J.Adams, STAR Collaboration","submitted_at":"2006-06-07T12:16:59Z","abstract_excerpt":"We present the scaling properties of Lambda, Xi, Omega and their anti-particles produced at mid-rapidity in Au+Au collisions at RHIC at sqrt(s_NN) = 200 GeV. The yield of multi-strange baryons per participant nucleon increases from peripheral to central collisions more rapidly than the Lambda yield, which appears to correspond to an increasing strange quark density of matter produced. The value of the strange phase space occupancy factor gamma_s, obtained from a thermal model fit to the data, approaches unity for the most central collisions. We also show that the nuclear modification factors, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0606014","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/0606014/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/0606014","created_at":"2026-07-04T15:26:11.126040+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-ex/0606014v1","created_at":"2026-07-04T15:26:11.126040+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-ex/0606014","created_at":"2026-07-04T15:26:11.126040+00:00"},{"alias_kind":"pith_short_12","alias_value":"7HPWOJB264BL","created_at":"2026-07-04T15:26:11.126040+00:00"},{"alias_kind":"pith_short_16","alias_value":"7HPWOJB264BLBT6K","created_at":"2026-07-04T15:26:11.126040+00:00"},{"alias_kind":"pith_short_8","alias_value":"7HPWOJB2","created_at":"2026-07-04T15:26:11.126040+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.05428","citing_title":"Disentangling Initial-State and Evolution Effects in Heavy-Ion Collisions Using EPOS and PHSD","ref_index":64,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7HPWOJB264BLBT6KZVAUGHD6H7","json":"https://pith.science/pith/7HPWOJB264BLBT6KZVAUGHD6H7.json","graph_json":"https://pith.science/api/pith-number/7HPWOJB264BLBT6KZVAUGHD6H7/graph.json","events_json":"https://pith.science/api/pith-number/7HPWOJB264BLBT6KZVAUGHD6H7/events.json","paper":"https://pith.science/paper/7HPWOJB2"},"agent_actions":{"view_html":"https://pith.science/pith/7HPWOJB264BLBT6KZVAUGHD6H7","download_json":"https://pith.science/pith/7HPWOJB264BLBT6KZVAUGHD6H7.json","view_paper":"https://pith.science/paper/7HPWOJB2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-ex/0606014&json=true","fetch_graph":"https://pith.science/api/pith-number/7HPWOJB264BLBT6KZVAUGHD6H7/graph.json","fetch_events":"https://pith.science/api/pith-number/7HPWOJB264BLBT6KZVAUGHD6H7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7HPWOJB264BLBT6KZVAUGHD6H7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7HPWOJB264BLBT6KZVAUGHD6H7/action/storage_attestation","attest_author":"https://pith.science/pith/7HPWOJB264BLBT6KZVAUGHD6H7/action/author_attestation","sign_citation":"https://pith.science/pith/7HPWOJB264BLBT6KZVAUGHD6H7/action/citation_signature","submit_replication":"https://pith.science/pith/7HPWOJB264BLBT6KZVAUGHD6H7/action/replication_record"}},"created_at":"2026-07-04T15:26:11.126040+00:00","updated_at":"2026-07-04T15:26:11.126040+00:00"}