{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:7G2JAQZU46A44PEGFYCEJNFNWZ","short_pith_number":"pith:7G2JAQZU","schema_version":"1.0","canonical_sha256":"f9b4904334e781ce3c862e0444b4adb65c34cadef939bf3f8542709882ea6a33","source":{"kind":"arxiv","id":"nucl-th/9901094","version":1},"attestation_state":"computed","paper":{"title":"Particle Interferometry for Relativistic Heavy-Ion Collisions","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Ulrich Heinz, Urs Achim Wiedemann","submitted_at":"1999-01-28T19:04:26Z","abstract_excerpt":"In this report we give a detailed account on Hanbury Brown/Twiss (HBT) particle interferometric methods for relativistic heavy-ion collisions. These exploit identical two-particle correlations to gain access to the space-time geometry and dynamics of the final freeze-out stage. The connection between the measured correlations in momentum space and the phase-space structure of the particle emitter is established, both with and without final state interactions. Suitable Gaussian parametrizations for the two-particle correlation function are derived and the physical interpretation of their parame"},"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/9901094","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1999-01-28T19:04:26Z","cross_cats_sorted":[],"title_canon_sha256":"64f4d2c18458993be450c8acd76ab2719cedc89f62e9ebe2bdbd65b79269240d","abstract_canon_sha256":"cae5ffd8b19fc120085a8c914e6dffa1960b91a3836d8761fac40abdb3158567"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:54:15.123132Z","signature_b64":"LSjGwxT28GoLKP3jhaHNEQRER44DIJ36z4YTbYR7qeJrxSlQ8oc4y2h9hC8KbMpgbYWTRP3z7jtLr0NzY2ydAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f9b4904334e781ce3c862e0444b4adb65c34cadef939bf3f8542709882ea6a33","last_reissued_at":"2026-07-04T15:54:15.122694Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:54:15.122694Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Particle Interferometry for Relativistic Heavy-Ion Collisions","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Ulrich Heinz, Urs Achim Wiedemann","submitted_at":"1999-01-28T19:04:26Z","abstract_excerpt":"In this report we give a detailed account on Hanbury Brown/Twiss (HBT) particle interferometric methods for relativistic heavy-ion collisions. These exploit identical two-particle correlations to gain access to the space-time geometry and dynamics of the final freeze-out stage. The connection between the measured correlations in momentum space and the phase-space structure of the particle emitter is established, both with and without final state interactions. Suitable Gaussian parametrizations for the two-particle correlation function are derived and the physical interpretation of their parame"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9901094","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/9901094/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/9901094","created_at":"2026-07-04T15:54:15.122759+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9901094v1","created_at":"2026-07-04T15:54:15.122759+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9901094","created_at":"2026-07-04T15:54:15.122759+00:00"},{"alias_kind":"pith_short_12","alias_value":"7G2JAQZU46A4","created_at":"2026-07-04T15:54:15.122759+00:00"},{"alias_kind":"pith_short_16","alias_value":"7G2JAQZU46A44PEG","created_at":"2026-07-04T15:54:15.122759+00:00"},{"alias_kind":"pith_short_8","alias_value":"7G2JAQZU","created_at":"2026-07-04T15:54:15.122759+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.19626","citing_title":"A self-consistent calculation of non-spherical Bose-Einstein correlation functions with Coulomb final-state interaction","ref_index":9,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7G2JAQZU46A44PEGFYCEJNFNWZ","json":"https://pith.science/pith/7G2JAQZU46A44PEGFYCEJNFNWZ.json","graph_json":"https://pith.science/api/pith-number/7G2JAQZU46A44PEGFYCEJNFNWZ/graph.json","events_json":"https://pith.science/api/pith-number/7G2JAQZU46A44PEGFYCEJNFNWZ/events.json","paper":"https://pith.science/paper/7G2JAQZU"},"agent_actions":{"view_html":"https://pith.science/pith/7G2JAQZU46A44PEGFYCEJNFNWZ","download_json":"https://pith.science/pith/7G2JAQZU46A44PEGFYCEJNFNWZ.json","view_paper":"https://pith.science/paper/7G2JAQZU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9901094&json=true","fetch_graph":"https://pith.science/api/pith-number/7G2JAQZU46A44PEGFYCEJNFNWZ/graph.json","fetch_events":"https://pith.science/api/pith-number/7G2JAQZU46A44PEGFYCEJNFNWZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7G2JAQZU46A44PEGFYCEJNFNWZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7G2JAQZU46A44PEGFYCEJNFNWZ/action/storage_attestation","attest_author":"https://pith.science/pith/7G2JAQZU46A44PEGFYCEJNFNWZ/action/author_attestation","sign_citation":"https://pith.science/pith/7G2JAQZU46A44PEGFYCEJNFNWZ/action/citation_signature","submit_replication":"https://pith.science/pith/7G2JAQZU46A44PEGFYCEJNFNWZ/action/replication_record"}},"created_at":"2026-07-04T15:54:15.122759+00:00","updated_at":"2026-07-04T15:54:15.122759+00:00"}