{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:RO2RAWZZQDOD7JEJCAXO573PTK","short_pith_number":"pith:RO2RAWZZ","schema_version":"1.0","canonical_sha256":"8bb5105b3980dc3fa489102eeeff6f9ab8494c5537ed54a8f497d93a4c0cbe41","source":{"kind":"arxiv","id":"hep-ph/0008326","version":3},"attestation_state":"computed","paper":{"title":"Resolving the Antibaryon-Production Puzzle in High-Energy Heavy-Ion Collisions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"E.V. Shuryak, R. Rapp","submitted_at":"2000-08-31T22:34:55Z","abstract_excerpt":"We argue that the observed antiproton production in heavy-ion collisions at CERN-SpS energies can be understood if (contrary to most sequential scattering approaches) the backward direction in the process $p\\bar p \\leftrightarrow \\bar{n}\\pi$ (with $\\bar{n}$=5-6) is consistently accounted for within a thermal framework. Employing the standard picture of subsequent chemical and thermal freezeout, which induces an over-saturation of pion number with associated chemical potentials of $\\mu_\\pi\\simeq$~60-80 MeV, enhances the backward reaction substantially. The resulting rates and corresponding cros"},"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/0008326","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2000-08-31T22:34:55Z","cross_cats_sorted":[],"title_canon_sha256":"231f471a0f7dbf8bbdbbcc932d5c178939e0ad9b777186920fdc10fc2e10d66a","abstract_canon_sha256":"f03853ff3cb08276a0f2f10611851aecd48c7965fd12923189690b0f388d44f9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:20:25.056752Z","signature_b64":"T0diJbFAGmudTONSyZwld94zbCBATVxMGVxkiGfnY92IiDH3l1T34xgnQqRsD5P3YNryiA87J01wd5GC+UgWBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8bb5105b3980dc3fa489102eeeff6f9ab8494c5537ed54a8f497d93a4c0cbe41","last_reissued_at":"2026-07-04T16:20:25.056374Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:20:25.056374Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resolving the Antibaryon-Production Puzzle in High-Energy Heavy-Ion Collisions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"E.V. Shuryak, R. Rapp","submitted_at":"2000-08-31T22:34:55Z","abstract_excerpt":"We argue that the observed antiproton production in heavy-ion collisions at CERN-SpS energies can be understood if (contrary to most sequential scattering approaches) the backward direction in the process $p\\bar p \\leftrightarrow \\bar{n}\\pi$ (with $\\bar{n}$=5-6) is consistently accounted for within a thermal framework. Employing the standard picture of subsequent chemical and thermal freezeout, which induces an over-saturation of pion number with associated chemical potentials of $\\mu_\\pi\\simeq$~60-80 MeV, enhances the backward reaction substantially. The resulting rates and corresponding cros"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0008326","kind":"arxiv","version":3},"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/hep-ph/0008326/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":"hep-ph/0008326","created_at":"2026-07-04T16:20:25.056443+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0008326v3","created_at":"2026-07-04T16:20:25.056443+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0008326","created_at":"2026-07-04T16:20:25.056443+00:00"},{"alias_kind":"pith_short_12","alias_value":"RO2RAWZZQDOD","created_at":"2026-07-04T16:20:25.056443+00:00"},{"alias_kind":"pith_short_16","alias_value":"RO2RAWZZQDOD7JEJ","created_at":"2026-07-04T16:20:25.056443+00:00"},{"alias_kind":"pith_short_8","alias_value":"RO2RAWZZ","created_at":"2026-07-04T16:20:25.056443+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.14884","citing_title":"Probing Late-Stage Hadronic Interactions at High Baryon Density via $K^{*0}$ Production in the RHIC Beam Energy Scan Program","ref_index":10,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RO2RAWZZQDOD7JEJCAXO573PTK","json":"https://pith.science/pith/RO2RAWZZQDOD7JEJCAXO573PTK.json","graph_json":"https://pith.science/api/pith-number/RO2RAWZZQDOD7JEJCAXO573PTK/graph.json","events_json":"https://pith.science/api/pith-number/RO2RAWZZQDOD7JEJCAXO573PTK/events.json","paper":"https://pith.science/paper/RO2RAWZZ"},"agent_actions":{"view_html":"https://pith.science/pith/RO2RAWZZQDOD7JEJCAXO573PTK","download_json":"https://pith.science/pith/RO2RAWZZQDOD7JEJCAXO573PTK.json","view_paper":"https://pith.science/paper/RO2RAWZZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0008326&json=true","fetch_graph":"https://pith.science/api/pith-number/RO2RAWZZQDOD7JEJCAXO573PTK/graph.json","fetch_events":"https://pith.science/api/pith-number/RO2RAWZZQDOD7JEJCAXO573PTK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RO2RAWZZQDOD7JEJCAXO573PTK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RO2RAWZZQDOD7JEJCAXO573PTK/action/storage_attestation","attest_author":"https://pith.science/pith/RO2RAWZZQDOD7JEJCAXO573PTK/action/author_attestation","sign_citation":"https://pith.science/pith/RO2RAWZZQDOD7JEJCAXO573PTK/action/citation_signature","submit_replication":"https://pith.science/pith/RO2RAWZZQDOD7JEJCAXO573PTK/action/replication_record"}},"created_at":"2026-07-04T16:20:25.056443+00:00","updated_at":"2026-07-04T16:20:25.056443+00:00"}