{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:N73UYIA7QTNSCKA2SCS2XYKJ7A","short_pith_number":"pith:N73UYIA7","schema_version":"1.0","canonical_sha256":"6ff74c201f84db21281a90a5abe149f80631584dab7fe4cbe176dad8ccc5491f","source":{"kind":"arxiv","id":"2110.13153","version":1},"attestation_state":"computed","paper":{"title":"Predictions and postdictions for relativistic lead and oxygen collisions with Trajectum","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Govert Nijs, Wilke van der Schee","submitted_at":"2021-10-25T18:00:00Z","abstract_excerpt":"We introduce a global analysis of relativistic heavy ion collisions using Trajectum of a significantly higher precision and including a new option to vary the normalization of the centrality estimator. We use the posterior distribution of our parameters to generate a set of high statistics samples that allows us to make precise predictions including statistical and systematic uncertainties estimated from the model parameter distribution. The results are systematically compared with experiment whereby we also include many observables not included in the global analysis. This includes in particu"},"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":"2110.13153","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2021-10-25T18:00:00Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"d892c3c0d30c0f16a8a06ef1400016e89c166a314db24f6e2279d0277b6f8e1d","abstract_canon_sha256":"47ecf2ac974949e02f48cc4f6e9e9967949b40154737059d95f4ccc55f6c29ff"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:25:35.692419Z","signature_b64":"iJ6XX6y3bjfDqqLWLSoJ65BCshA7tHFUVzdy5Dyit1K9q6OGHoQnYjnuUChXz5607d1nV/ejHhZoqQ9QAxkbBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ff74c201f84db21281a90a5abe149f80631584dab7fe4cbe176dad8ccc5491f","last_reissued_at":"2026-07-05T03:25:35.691977Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:25:35.691977Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Predictions and postdictions for relativistic lead and oxygen collisions with Trajectum","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Govert Nijs, Wilke van der Schee","submitted_at":"2021-10-25T18:00:00Z","abstract_excerpt":"We introduce a global analysis of relativistic heavy ion collisions using Trajectum of a significantly higher precision and including a new option to vary the normalization of the centrality estimator. We use the posterior distribution of our parameters to generate a set of high statistics samples that allows us to make precise predictions including statistical and systematic uncertainties estimated from the model parameter distribution. The results are systematically compared with experiment whereby we also include many observables not included in the global analysis. This includes in particu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.13153","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/2110.13153/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":"2110.13153","created_at":"2026-07-05T03:25:35.692033+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.13153v1","created_at":"2026-07-05T03:25:35.692033+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.13153","created_at":"2026-07-05T03:25:35.692033+00:00"},{"alias_kind":"pith_short_12","alias_value":"N73UYIA7QTNS","created_at":"2026-07-05T03:25:35.692033+00:00"},{"alias_kind":"pith_short_16","alias_value":"N73UYIA7QTNSCKA2","created_at":"2026-07-05T03:25:35.692033+00:00"},{"alias_kind":"pith_short_8","alias_value":"N73UYIA7","created_at":"2026-07-05T03:25:35.692033+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.20257","citing_title":"Measurements of charged-particle pseudorapidity and transverse momentum distributions in O+O and Ne+Ne collisions at $\\sqrt{s_{_\\text{NN}}} = 5.36$ TeV with the ATLAS detector","ref_index":62,"is_internal_anchor":false},{"citing_arxiv_id":"2509.05171","citing_title":"Measurement of the azimuthal anisotropy of charged particles in $\\sqrt{s_{\\mathrm{NN}}}=5.36$ TeV $^{16}$O$+^{16}$O and $^{20}$Ne$+^{20}$Ne collisions with the ATLAS detector","ref_index":86,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/N73UYIA7QTNSCKA2SCS2XYKJ7A","json":"https://pith.science/pith/N73UYIA7QTNSCKA2SCS2XYKJ7A.json","graph_json":"https://pith.science/api/pith-number/N73UYIA7QTNSCKA2SCS2XYKJ7A/graph.json","events_json":"https://pith.science/api/pith-number/N73UYIA7QTNSCKA2SCS2XYKJ7A/events.json","paper":"https://pith.science/paper/N73UYIA7"},"agent_actions":{"view_html":"https://pith.science/pith/N73UYIA7QTNSCKA2SCS2XYKJ7A","download_json":"https://pith.science/pith/N73UYIA7QTNSCKA2SCS2XYKJ7A.json","view_paper":"https://pith.science/paper/N73UYIA7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.13153&json=true","fetch_graph":"https://pith.science/api/pith-number/N73UYIA7QTNSCKA2SCS2XYKJ7A/graph.json","fetch_events":"https://pith.science/api/pith-number/N73UYIA7QTNSCKA2SCS2XYKJ7A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N73UYIA7QTNSCKA2SCS2XYKJ7A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N73UYIA7QTNSCKA2SCS2XYKJ7A/action/storage_attestation","attest_author":"https://pith.science/pith/N73UYIA7QTNSCKA2SCS2XYKJ7A/action/author_attestation","sign_citation":"https://pith.science/pith/N73UYIA7QTNSCKA2SCS2XYKJ7A/action/citation_signature","submit_replication":"https://pith.science/pith/N73UYIA7QTNSCKA2SCS2XYKJ7A/action/replication_record"}},"created_at":"2026-07-05T03:25:35.692033+00:00","updated_at":"2026-07-05T03:25:35.692033+00:00"}