{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:OG7XZ6T63E3LB4H33LEQDXXM6R","short_pith_number":"pith:OG7XZ6T6","schema_version":"1.0","canonical_sha256":"71bf7cfa7ed936b0f0fbdac901deecf4593b289a7ec15884f7e23e1a4f06df30","source":{"kind":"arxiv","id":"nucl-th/9902062","version":2},"attestation_state":"computed","paper":{"title":"Hadronic freeze-out following a first order hadronization phase transition in ultrarelativistic heavy-ion collisions","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"A. Dumitru, E. Zabrodin, H. Stoecker, L. Bravina, M. Bleicher, S.A. Bass, W. Greiner","submitted_at":"1999-02-23T16:56:59Z","abstract_excerpt":"We analyze the hadronic freeze-out in ultra-relativistic heavy ion collisions at RHIC in a transport approach which combines hydrodynamics for the early, dense, deconfined stage of the reaction with a microscopic non-equilibrium model for the later hadronic stage at which the hydrodynamic equilibrium assumptions are not valid. With this ansatz we are able to self-consistently calculate the freeze-out of the system and determine space-time hypersurfaces for individual hadron species. The space-time domains of the freeze-out for several hadron species are found to be actually four-dimensional, a"},"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-th/9902062","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1999-02-23T16:56:59Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"b0200db0fb68c52dc3df50b995761125a1463038a02dbcdb157421154a60a4e7","abstract_canon_sha256":"ef536687b9e167efe2cd1d67929514ff5972d93b232a5ece12294466ac32e264"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:23:29.599743Z","signature_b64":"SPLtpPQcH80i+HO/vtTLhjBsvJlDvYrX1wCHZWFEihI22m/j1QpB21YCGLQoy23nuIdjSGFRX1bA8MM1OLvrDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"71bf7cfa7ed936b0f0fbdac901deecf4593b289a7ec15884f7e23e1a4f06df30","last_reissued_at":"2026-07-04T15:23:29.599330Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:23:29.599330Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hadronic freeze-out following a first order hadronization phase transition in ultrarelativistic heavy-ion collisions","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"A. Dumitru, E. Zabrodin, H. Stoecker, L. Bravina, M. Bleicher, S.A. Bass, W. Greiner","submitted_at":"1999-02-23T16:56:59Z","abstract_excerpt":"We analyze the hadronic freeze-out in ultra-relativistic heavy ion collisions at RHIC in a transport approach which combines hydrodynamics for the early, dense, deconfined stage of the reaction with a microscopic non-equilibrium model for the later hadronic stage at which the hydrodynamic equilibrium assumptions are not valid. With this ansatz we are able to self-consistently calculate the freeze-out of the system and determine space-time hypersurfaces for individual hadron species. The space-time domains of the freeze-out for several hadron species are found to be actually four-dimensional, a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9902062","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/nucl-th/9902062/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-th/9902062","created_at":"2026-07-04T15:23:29.599397+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9902062v2","created_at":"2026-07-04T15:23:29.599397+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9902062","created_at":"2026-07-04T15:23:29.599397+00:00"},{"alias_kind":"pith_short_12","alias_value":"OG7XZ6T63E3L","created_at":"2026-07-04T15:23:29.599397+00:00"},{"alias_kind":"pith_short_16","alias_value":"OG7XZ6T63E3LB4H3","created_at":"2026-07-04T15:23:29.599397+00:00"},{"alias_kind":"pith_short_8","alias_value":"OG7XZ6T6","created_at":"2026-07-04T15:23:29.599397+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.24777","citing_title":"Mass-Dependent Non-Extensivity in Tsallis Blast-Wave Fits to Identified Hadron $p_T$ Spectra at RHIC and LHC","ref_index":48,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OG7XZ6T63E3LB4H33LEQDXXM6R","json":"https://pith.science/pith/OG7XZ6T63E3LB4H33LEQDXXM6R.json","graph_json":"https://pith.science/api/pith-number/OG7XZ6T63E3LB4H33LEQDXXM6R/graph.json","events_json":"https://pith.science/api/pith-number/OG7XZ6T63E3LB4H33LEQDXXM6R/events.json","paper":"https://pith.science/paper/OG7XZ6T6"},"agent_actions":{"view_html":"https://pith.science/pith/OG7XZ6T63E3LB4H33LEQDXXM6R","download_json":"https://pith.science/pith/OG7XZ6T63E3LB4H33LEQDXXM6R.json","view_paper":"https://pith.science/paper/OG7XZ6T6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9902062&json=true","fetch_graph":"https://pith.science/api/pith-number/OG7XZ6T63E3LB4H33LEQDXXM6R/graph.json","fetch_events":"https://pith.science/api/pith-number/OG7XZ6T63E3LB4H33LEQDXXM6R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OG7XZ6T63E3LB4H33LEQDXXM6R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OG7XZ6T63E3LB4H33LEQDXXM6R/action/storage_attestation","attest_author":"https://pith.science/pith/OG7XZ6T63E3LB4H33LEQDXXM6R/action/author_attestation","sign_citation":"https://pith.science/pith/OG7XZ6T63E3LB4H33LEQDXXM6R/action/citation_signature","submit_replication":"https://pith.science/pith/OG7XZ6T63E3LB4H33LEQDXXM6R/action/replication_record"}},"created_at":"2026-07-04T15:23:29.599397+00:00","updated_at":"2026-07-04T15:23:29.599397+00:00"}