{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:KSDRBRX42KPITY3NHKRA4CAHB4","short_pith_number":"pith:KSDRBRX4","schema_version":"1.0","canonical_sha256":"548710c6fcd29e89e36d3aa20e08070f3a832a4e6ab180d67510f3adb92dd595","source":{"kind":"arxiv","id":"2508.11897","version":1},"attestation_state":"computed","paper":{"title":"Simulation of heavy quarkonium equilibration in the quark-gluon plasma","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Min He, Shouxing Zhao","submitted_at":"2025-08-16T04:01:53Z","abstract_excerpt":"We simulate the heavy quarkonium equilibration through transport in a static and homogeneous quark-gluon plasma (QGP) box within the semi-classical Boltzmann approach incorporating both the leading-order and next-to-leading-order dissociation and regeneration reactions. The scattering amplitudes involved are taken from perturbative computations based on effective color-electric dipole coupling of the heavy quarkonium with thermal gluons. By coupling the Langevin simulation of single heavy quark diffusion and the Boltzmann transport of the heavy quarkonium in a real-time fashion, we demonstrate"},"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":"2508.11897","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2025-08-16T04:01:53Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"b1b6d0201bf8850de824e54dad33dd6b1f28bcd2306c250314021db86e3c49e2","abstract_canon_sha256":"6391191379fa5c55e1088d36d33146d5253878c68ac96ac199c2bb411d0cefe5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:54:56.654327Z","signature_b64":"/yms8zP8OiftmxT7Su+XLLd0pK1Ymr/mWXicOmjSK6Q2Qj98pgJ9jRX55vsYyTGiC5oIsWyzhq5evCIIZQ2yCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"548710c6fcd29e89e36d3aa20e08070f3a832a4e6ab180d67510f3adb92dd595","last_reissued_at":"2026-07-05T11:54:56.653780Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:54:56.653780Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simulation of heavy quarkonium equilibration in the quark-gluon plasma","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Min He, Shouxing Zhao","submitted_at":"2025-08-16T04:01:53Z","abstract_excerpt":"We simulate the heavy quarkonium equilibration through transport in a static and homogeneous quark-gluon plasma (QGP) box within the semi-classical Boltzmann approach incorporating both the leading-order and next-to-leading-order dissociation and regeneration reactions. The scattering amplitudes involved are taken from perturbative computations based on effective color-electric dipole coupling of the heavy quarkonium with thermal gluons. By coupling the Langevin simulation of single heavy quark diffusion and the Boltzmann transport of the heavy quarkonium in a real-time fashion, we demonstrate"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.11897","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/2508.11897/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":"2508.11897","created_at":"2026-07-05T11:54:56.653846+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.11897v1","created_at":"2026-07-05T11:54:56.653846+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.11897","created_at":"2026-07-05T11:54:56.653846+00:00"},{"alias_kind":"pith_short_12","alias_value":"KSDRBRX42KPI","created_at":"2026-07-05T11:54:56.653846+00:00"},{"alias_kind":"pith_short_16","alias_value":"KSDRBRX42KPITY3N","created_at":"2026-07-05T11:54:56.653846+00:00"},{"alias_kind":"pith_short_8","alias_value":"KSDRBRX4","created_at":"2026-07-05T11:54:56.653846+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/KSDRBRX42KPITY3NHKRA4CAHB4","json":"https://pith.science/pith/KSDRBRX42KPITY3NHKRA4CAHB4.json","graph_json":"https://pith.science/api/pith-number/KSDRBRX42KPITY3NHKRA4CAHB4/graph.json","events_json":"https://pith.science/api/pith-number/KSDRBRX42KPITY3NHKRA4CAHB4/events.json","paper":"https://pith.science/paper/KSDRBRX4"},"agent_actions":{"view_html":"https://pith.science/pith/KSDRBRX42KPITY3NHKRA4CAHB4","download_json":"https://pith.science/pith/KSDRBRX42KPITY3NHKRA4CAHB4.json","view_paper":"https://pith.science/paper/KSDRBRX4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.11897&json=true","fetch_graph":"https://pith.science/api/pith-number/KSDRBRX42KPITY3NHKRA4CAHB4/graph.json","fetch_events":"https://pith.science/api/pith-number/KSDRBRX42KPITY3NHKRA4CAHB4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KSDRBRX42KPITY3NHKRA4CAHB4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KSDRBRX42KPITY3NHKRA4CAHB4/action/storage_attestation","attest_author":"https://pith.science/pith/KSDRBRX42KPITY3NHKRA4CAHB4/action/author_attestation","sign_citation":"https://pith.science/pith/KSDRBRX42KPITY3NHKRA4CAHB4/action/citation_signature","submit_replication":"https://pith.science/pith/KSDRBRX42KPITY3NHKRA4CAHB4/action/replication_record"}},"created_at":"2026-07-05T11:54:56.653846+00:00","updated_at":"2026-07-05T11:54:56.653846+00:00"}