{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:Y7H77TGPQORYWULNDDAIKMV5AV","short_pith_number":"pith:Y7H77TGP","schema_version":"1.0","canonical_sha256":"c7cfffcccf83a38b516d18c08532bd056eae8b1f807df0d48a2575d38e4f9937","source":{"kind":"arxiv","id":"hep-ph/0306077","version":2},"attestation_state":"computed","paper":{"title":"In-Medium Effects on Charmonium Production in Heavy-Ion Collisions","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"G. E. Brown, L. Grandchamp, R. Rapp","submitted_at":"2003-06-09T19:08:34Z","abstract_excerpt":"Charmonium production in heavy-ion collisions is investigated within a kinetic theory framework incorporating in-medium properties of open- and hidden-charm states in line with recent QCD lattice calculations. A continuously decreasing open-charm threshold across the phase boundary of hadronic and quark-gluon matter is found to have important implications for the equilibrium abundance of charmonium states. The survival of $J/\\psi$ resonance states above the transition temperature enables their recreation also in the Quark-Gluon Plasma. Including effects of chemical and thermal off-equilibrium,"},"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/0306077","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-06-09T19:08:34Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"a29273dfad7115275a2d778efbef289604ca115c9d3fefdf32451c4d6e526b15","abstract_canon_sha256":"1bdc1a7ceff6bee32f81df8afd5f34c9cc0debfa44018e43d6f5be949d4c38de"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:22:59.862154Z","signature_b64":"MkvhfVy5sijMKXFJkEP0ZByDnyfLDcuTgqP+fzDYVUMgqH91jNsPkin9CTywbb87LzKaTz4VlDPgIeiW89H7BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c7cfffcccf83a38b516d18c08532bd056eae8b1f807df0d48a2575d38e4f9937","last_reissued_at":"2026-05-18T04:22:59.861508Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:22:59.861508Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"In-Medium Effects on Charmonium Production in Heavy-Ion Collisions","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"G. E. Brown, L. Grandchamp, R. Rapp","submitted_at":"2003-06-09T19:08:34Z","abstract_excerpt":"Charmonium production in heavy-ion collisions is investigated within a kinetic theory framework incorporating in-medium properties of open- and hidden-charm states in line with recent QCD lattice calculations. A continuously decreasing open-charm threshold across the phase boundary of hadronic and quark-gluon matter is found to have important implications for the equilibrium abundance of charmonium states. The survival of $J/\\psi$ resonance states above the transition temperature enables their recreation also in the Quark-Gluon Plasma. Including effects of chemical and thermal off-equilibrium,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0306077","kind":"arxiv","version":2},"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/0306077","created_at":"2026-05-18T04:22:59.861604+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0306077v2","created_at":"2026-05-18T04:22:59.861604+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0306077","created_at":"2026-05-18T04:22:59.861604+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y7H77TGPQORY","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y7H77TGPQORYWULN","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y7H77TGP","created_at":"2026-05-18T12:25:52.051335+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.20995","citing_title":"Bottomonium transport in a strongly coupled quark-gluon plasma","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2604.09198","citing_title":"Unified Extraction of In-Medium Heavy Quark Potentials from RHIC to LHC Energies via Deep Learning","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Y7H77TGPQORYWULNDDAIKMV5AV","json":"https://pith.science/pith/Y7H77TGPQORYWULNDDAIKMV5AV.json","graph_json":"https://pith.science/api/pith-number/Y7H77TGPQORYWULNDDAIKMV5AV/graph.json","events_json":"https://pith.science/api/pith-number/Y7H77TGPQORYWULNDDAIKMV5AV/events.json","paper":"https://pith.science/paper/Y7H77TGP"},"agent_actions":{"view_html":"https://pith.science/pith/Y7H77TGPQORYWULNDDAIKMV5AV","download_json":"https://pith.science/pith/Y7H77TGPQORYWULNDDAIKMV5AV.json","view_paper":"https://pith.science/paper/Y7H77TGP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0306077&json=true","fetch_graph":"https://pith.science/api/pith-number/Y7H77TGPQORYWULNDDAIKMV5AV/graph.json","fetch_events":"https://pith.science/api/pith-number/Y7H77TGPQORYWULNDDAIKMV5AV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y7H77TGPQORYWULNDDAIKMV5AV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y7H77TGPQORYWULNDDAIKMV5AV/action/storage_attestation","attest_author":"https://pith.science/pith/Y7H77TGPQORYWULNDDAIKMV5AV/action/author_attestation","sign_citation":"https://pith.science/pith/Y7H77TGPQORYWULNDDAIKMV5AV/action/citation_signature","submit_replication":"https://pith.science/pith/Y7H77TGPQORYWULNDDAIKMV5AV/action/replication_record"}},"created_at":"2026-05-18T04:22:59.861604+00:00","updated_at":"2026-05-18T04:22:59.861604+00:00"}