{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:EXXOZFDERLVJ5WGEBS2SC7ARKW","short_pith_number":"pith:EXXOZFDE","schema_version":"1.0","canonical_sha256":"25eeec94648aea9ed8c40cb5217c115593c01c64c2150f10fbeb3dc1b7720667","source":{"kind":"arxiv","id":"nucl-th/9606039","version":1},"attestation_state":"computed","paper":{"title":"The Time-Delay Signature of Quark-Gluon-Plasma Formation in Relativistic Nuclear Collisions","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Dirk H. Rischke, Miklos Gyulassy","submitted_at":"1996-06-19T21:12:51Z","abstract_excerpt":"The hydrodynamic expansion of quark-gluon plasmas with spherical and longitudinally boost-invariant geometries is studied as a function of the initial energy density. The sensitivity of the collective flow pattern to uncertainties in the nuclear matter equation of state is explored. We concentrate on the effect of a possible finite width, $\\Delta T \\sim 0.1 T_c$, of the transition region between quark-gluon plasma and hadronic phase. Although slow deflagration solutions that act to stall the expansion do not exist for $\\Delta T > 0.08 T_c$, we find, nevertheless, that the equation of state rem"},"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/9606039","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1996-06-19T21:12:51Z","cross_cats_sorted":[],"title_canon_sha256":"a35a26edb1be3f0cb215ce4477801e2f00b410617de7f34c0cc4fe0c3253996d","abstract_canon_sha256":"449270a9a24c657b660d6135f1cb330799ab2a520907d90b4a591745bd52a418"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:54:14.632228Z","signature_b64":"AYnyszG0M1NFjLTz8hds6pO8BHFHIrA1MdlyZsoVfZV5yq+4Npns0lK/Xk3NVh6inYC1angVz9QlAY1D3qpqDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"25eeec94648aea9ed8c40cb5217c115593c01c64c2150f10fbeb3dc1b7720667","last_reissued_at":"2026-07-04T15:54:14.631743Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:54:14.631743Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Time-Delay Signature of Quark-Gluon-Plasma Formation in Relativistic Nuclear Collisions","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Dirk H. Rischke, Miklos Gyulassy","submitted_at":"1996-06-19T21:12:51Z","abstract_excerpt":"The hydrodynamic expansion of quark-gluon plasmas with spherical and longitudinally boost-invariant geometries is studied as a function of the initial energy density. The sensitivity of the collective flow pattern to uncertainties in the nuclear matter equation of state is explored. We concentrate on the effect of a possible finite width, $\\Delta T \\sim 0.1 T_c$, of the transition region between quark-gluon plasma and hadronic phase. Although slow deflagration solutions that act to stall the expansion do not exist for $\\Delta T > 0.08 T_c$, we find, nevertheless, that the equation of state rem"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9606039","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/9606039/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/9606039","created_at":"2026-07-04T15:54:14.631804+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9606039v1","created_at":"2026-07-04T15:54:14.631804+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9606039","created_at":"2026-07-04T15:54:14.631804+00:00"},{"alias_kind":"pith_short_12","alias_value":"EXXOZFDERLVJ","created_at":"2026-07-04T15:54:14.631804+00:00"},{"alias_kind":"pith_short_16","alias_value":"EXXOZFDERLVJ5WGE","created_at":"2026-07-04T15:54:14.631804+00:00"},{"alias_kind":"pith_short_8","alias_value":"EXXOZFDE","created_at":"2026-07-04T15:54:14.631804+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":21,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EXXOZFDERLVJ5WGEBS2SC7ARKW","json":"https://pith.science/pith/EXXOZFDERLVJ5WGEBS2SC7ARKW.json","graph_json":"https://pith.science/api/pith-number/EXXOZFDERLVJ5WGEBS2SC7ARKW/graph.json","events_json":"https://pith.science/api/pith-number/EXXOZFDERLVJ5WGEBS2SC7ARKW/events.json","paper":"https://pith.science/paper/EXXOZFDE"},"agent_actions":{"view_html":"https://pith.science/pith/EXXOZFDERLVJ5WGEBS2SC7ARKW","download_json":"https://pith.science/pith/EXXOZFDERLVJ5WGEBS2SC7ARKW.json","view_paper":"https://pith.science/paper/EXXOZFDE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9606039&json=true","fetch_graph":"https://pith.science/api/pith-number/EXXOZFDERLVJ5WGEBS2SC7ARKW/graph.json","fetch_events":"https://pith.science/api/pith-number/EXXOZFDERLVJ5WGEBS2SC7ARKW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EXXOZFDERLVJ5WGEBS2SC7ARKW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EXXOZFDERLVJ5WGEBS2SC7ARKW/action/storage_attestation","attest_author":"https://pith.science/pith/EXXOZFDERLVJ5WGEBS2SC7ARKW/action/author_attestation","sign_citation":"https://pith.science/pith/EXXOZFDERLVJ5WGEBS2SC7ARKW/action/citation_signature","submit_replication":"https://pith.science/pith/EXXOZFDERLVJ5WGEBS2SC7ARKW/action/replication_record"}},"created_at":"2026-07-04T15:54:14.631804+00:00","updated_at":"2026-07-04T15:54:14.631804+00:00"}