{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:PEY2VKLAQOQE7VMPSO2G72H3LF","short_pith_number":"pith:PEY2VKLA","schema_version":"1.0","canonical_sha256":"7931aaa96083a04fd58f93b46fe8fb594c5bdb9cf0ba98d1811c12169d648538","source":{"kind":"arxiv","id":"nucl-th/0304079","version":1},"attestation_state":"computed","paper":{"title":"Blast-wave snapshots from RHIC","license":"","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Boris Tomasik","submitted_at":"2003-04-25T07:53:14Z","abstract_excerpt":"I present fits with the so-called blast-wave model to single-particle spectra and HBT correlations from Au+Au collisions at a CMS energy of 130 AGeV. There is only little choice of freeze-out temperature and transverse flow velocity for which the model fits both the identified spectra and the correlation radii just well enough not to be excluded. The observed steep M_t dependence of R_side leads to a temperature which it is problematic to interpret. The applicability of the model for the freeze-out description is thus questioned."},"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/0304079","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2003-04-25T07:53:14Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"55e090d0374aca2d5dd7cc2021006cb83f4b8ed3d9b07d83e9afd1f8634ede4e","abstract_canon_sha256":"b6d8c90d4c7711d574dc36540913e060324bf73f3619fec124822ad0d5e8335c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:42:32.267185Z","signature_b64":"U597Br96ALHliPv+Ee4urixGl+deN50TwaUKSeqAHsCj1tXCeGpEHv0lGvxRcElEunUVTimTjKnmhiunS+4bAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7931aaa96083a04fd58f93b46fe8fb594c5bdb9cf0ba98d1811c12169d648538","last_reissued_at":"2026-07-04T14:42:32.266765Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:42:32.266765Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Blast-wave snapshots from RHIC","license":"","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Boris Tomasik","submitted_at":"2003-04-25T07:53:14Z","abstract_excerpt":"I present fits with the so-called blast-wave model to single-particle spectra and HBT correlations from Au+Au collisions at a CMS energy of 130 AGeV. There is only little choice of freeze-out temperature and transverse flow velocity for which the model fits both the identified spectra and the correlation radii just well enough not to be excluded. The observed steep M_t dependence of R_side leads to a temperature which it is problematic to interpret. The applicability of the model for the freeze-out description is thus questioned."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0304079","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-th/0304079/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/0304079","created_at":"2026-07-04T14:42:32.266829+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0304079v1","created_at":"2026-07-04T14:42:32.266829+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0304079","created_at":"2026-07-04T14:42:32.266829+00:00"},{"alias_kind":"pith_short_12","alias_value":"PEY2VKLAQOQE","created_at":"2026-07-04T14:42:32.266829+00:00"},{"alias_kind":"pith_short_16","alias_value":"PEY2VKLAQOQE7VMP","created_at":"2026-07-04T14:42:32.266829+00:00"},{"alias_kind":"pith_short_8","alias_value":"PEY2VKLA","created_at":"2026-07-04T14:42:32.266829+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.07410","citing_title":"Finite Volume Effects on Transverse Momentum Spectra at LHC and RHIC Using a Blast-Wave Model with Planck Transformed Temperatures","ref_index":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PEY2VKLAQOQE7VMPSO2G72H3LF","json":"https://pith.science/pith/PEY2VKLAQOQE7VMPSO2G72H3LF.json","graph_json":"https://pith.science/api/pith-number/PEY2VKLAQOQE7VMPSO2G72H3LF/graph.json","events_json":"https://pith.science/api/pith-number/PEY2VKLAQOQE7VMPSO2G72H3LF/events.json","paper":"https://pith.science/paper/PEY2VKLA"},"agent_actions":{"view_html":"https://pith.science/pith/PEY2VKLAQOQE7VMPSO2G72H3LF","download_json":"https://pith.science/pith/PEY2VKLAQOQE7VMPSO2G72H3LF.json","view_paper":"https://pith.science/paper/PEY2VKLA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0304079&json=true","fetch_graph":"https://pith.science/api/pith-number/PEY2VKLAQOQE7VMPSO2G72H3LF/graph.json","fetch_events":"https://pith.science/api/pith-number/PEY2VKLAQOQE7VMPSO2G72H3LF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PEY2VKLAQOQE7VMPSO2G72H3LF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PEY2VKLAQOQE7VMPSO2G72H3LF/action/storage_attestation","attest_author":"https://pith.science/pith/PEY2VKLAQOQE7VMPSO2G72H3LF/action/author_attestation","sign_citation":"https://pith.science/pith/PEY2VKLAQOQE7VMPSO2G72H3LF/action/citation_signature","submit_replication":"https://pith.science/pith/PEY2VKLAQOQE7VMPSO2G72H3LF/action/replication_record"}},"created_at":"2026-07-04T14:42:32.266829+00:00","updated_at":"2026-07-04T14:42:32.266829+00:00"}