{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:SKGOWQV2ME7UII3PM4LD2EGROL","short_pith_number":"pith:SKGOWQV2","schema_version":"1.0","canonical_sha256":"928ceb42ba613f44236f67163d10d172ecbdd9973e8609d64550571b10009695","source":{"kind":"arxiv","id":"hep-ph/9806207","version":1},"attestation_state":"computed","paper":{"title":"Supercooling of rapidly expanding quark-gluon plasma","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"2, 2), 4), Bergen, E.E. Zabrodin (1, Frankfurt, Germany (2) Institute for Nuclear Physics, H. St\\\"ocker (1), L.P. Csernai (3), L.V. Bravina (1, Moscow, Moscow State University, Norway; (4) Alexander von Humboldt Fellow), Russia (3) Department of Physics, University of Bergen, University of Frankfurt, W. Greiner (1) ((1) Institute for Theoretical Physics","submitted_at":"1998-05-31T17:51:30Z","abstract_excerpt":"We reexamine the scenario of homogeneous nucleation of the quark-gluon plasma produced in ultra-relativistic heavy ion collisions. A generalization of the standard nucleation theory to rapidly expanding system is proposed. The nucleation rate is derived via the new scaling parameter $\\lambda_Z$. It is shown that the size distribution of hadronic clusters plays an important role in the dynamics of the phase transition. The longitudinally expanding system is supercooled to about 3-6%, then it is reheated, and the hadronization is completed within 6-10 fm/c, i.e. 5-10 times faster than it was est"},"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":"hep-ph/9806207","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-05-31T17:51:30Z","cross_cats_sorted":[],"title_canon_sha256":"22431c81bcb8677aa4b7bf9ae64bb65d2e4fd95e982badbbfb52ffe72308b491","abstract_canon_sha256":"43c2bcad480be2a1e5a05e69348f4ab8bb003d7577b86443daaee3b0e4ca449e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:16.585236Z","signature_b64":"j2eGidni0W8jBrvWydIgIt9+3ATyvbvx/NESfi/9fn2sjNOk6UKdb7E2NrdmrVz466iKA+r4STp3xr1Vo8/gBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"928ceb42ba613f44236f67163d10d172ecbdd9973e8609d64550571b10009695","last_reissued_at":"2026-05-18T01:09:16.584556Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:16.584556Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Supercooling of rapidly expanding quark-gluon plasma","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"2, 2), 4), Bergen, E.E. Zabrodin (1, Frankfurt, Germany (2) Institute for Nuclear Physics, H. St\\\"ocker (1), L.P. Csernai (3), L.V. Bravina (1, Moscow, Moscow State University, Norway; (4) Alexander von Humboldt Fellow), Russia (3) Department of Physics, University of Bergen, University of Frankfurt, W. Greiner (1) ((1) Institute for Theoretical Physics","submitted_at":"1998-05-31T17:51:30Z","abstract_excerpt":"We reexamine the scenario of homogeneous nucleation of the quark-gluon plasma produced in ultra-relativistic heavy ion collisions. A generalization of the standard nucleation theory to rapidly expanding system is proposed. The nucleation rate is derived via the new scaling parameter $\\lambda_Z$. It is shown that the size distribution of hadronic clusters plays an important role in the dynamics of the phase transition. The longitudinally expanding system is supercooled to about 3-6%, then it is reheated, and the hadronization is completed within 6-10 fm/c, i.e. 5-10 times faster than it was est"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9806207","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":""},"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":"hep-ph/9806207","created_at":"2026-05-18T01:09:16.584663+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9806207v1","created_at":"2026-05-18T01:09:16.584663+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9806207","created_at":"2026-05-18T01:09:16.584663+00:00"},{"alias_kind":"pith_short_12","alias_value":"SKGOWQV2ME7U","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_16","alias_value":"SKGOWQV2ME7UII3P","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_8","alias_value":"SKGOWQV2","created_at":"2026-05-18T12:25:49.038998+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SKGOWQV2ME7UII3PM4LD2EGROL","json":"https://pith.science/pith/SKGOWQV2ME7UII3PM4LD2EGROL.json","graph_json":"https://pith.science/api/pith-number/SKGOWQV2ME7UII3PM4LD2EGROL/graph.json","events_json":"https://pith.science/api/pith-number/SKGOWQV2ME7UII3PM4LD2EGROL/events.json","paper":"https://pith.science/paper/SKGOWQV2"},"agent_actions":{"view_html":"https://pith.science/pith/SKGOWQV2ME7UII3PM4LD2EGROL","download_json":"https://pith.science/pith/SKGOWQV2ME7UII3PM4LD2EGROL.json","view_paper":"https://pith.science/paper/SKGOWQV2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9806207&json=true","fetch_graph":"https://pith.science/api/pith-number/SKGOWQV2ME7UII3PM4LD2EGROL/graph.json","fetch_events":"https://pith.science/api/pith-number/SKGOWQV2ME7UII3PM4LD2EGROL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SKGOWQV2ME7UII3PM4LD2EGROL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SKGOWQV2ME7UII3PM4LD2EGROL/action/storage_attestation","attest_author":"https://pith.science/pith/SKGOWQV2ME7UII3PM4LD2EGROL/action/author_attestation","sign_citation":"https://pith.science/pith/SKGOWQV2ME7UII3PM4LD2EGROL/action/citation_signature","submit_replication":"https://pith.science/pith/SKGOWQV2ME7UII3PM4LD2EGROL/action/replication_record"}},"created_at":"2026-05-18T01:09:16.584663+00:00","updated_at":"2026-05-18T01:09:16.584663+00:00"}