{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:WSAUKK3RH7F2UC2BW4I2AEGJTB","short_pith_number":"pith:WSAUKK3R","schema_version":"1.0","canonical_sha256":"b481452b713fcbaa0b41b711a010c9986bbb77c79c395f7a224d6f0c1f8c3685","source":{"kind":"arxiv","id":"2306.02530","version":2},"attestation_state":"computed","paper":{"title":"Heavy quark drag and diffusion coefficients in the pre-hydrodynamic QCD plasma","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Xiaojian Du","submitted_at":"2023-06-05T01:36:22Z","abstract_excerpt":"Kinetic and chemical equilibrations play important roles in the formation of the quark-gluon plasma (QGP) in relativistic heavy-ion collisions (HICs). These processes further influence the production of hard and electromagnetic probes in HICs, in particular, the thermalization of heavy quarks, which are produced at an extremely early time before the formation of the QGP. We calculate the drag and diffusion coefficients of heavy quarks in the pre-hydrodynamic quantum chromodynamic (QCD) plasma with the state-of-the-art QCD effective kinetic theory (EKT) solver. We present the time, momentum, an"},"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":"2306.02530","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-06-05T01:36:22Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"12999ca2e241155cd6b43f780576dbe7a0f6311c0ceca790ea22a05a48c852e1","abstract_canon_sha256":"f12eaf127a36b8e5fb91d1b65a9793cf10362b4d9d05e21f402c2d2c933983bb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:21:11.218705Z","signature_b64":"Muy/YCjMafpKHpH7OsbgKyXBSNKteFZjr4aFquyios5N/Grc1z6aDhg4A66YCt02KCg6/JQEQJerevUXmhomCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b481452b713fcbaa0b41b711a010c9986bbb77c79c395f7a224d6f0c1f8c3685","last_reissued_at":"2026-07-05T07:21:11.218211Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:21:11.218211Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy quark drag and diffusion coefficients in the pre-hydrodynamic QCD plasma","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Xiaojian Du","submitted_at":"2023-06-05T01:36:22Z","abstract_excerpt":"Kinetic and chemical equilibrations play important roles in the formation of the quark-gluon plasma (QGP) in relativistic heavy-ion collisions (HICs). These processes further influence the production of hard and electromagnetic probes in HICs, in particular, the thermalization of heavy quarks, which are produced at an extremely early time before the formation of the QGP. We calculate the drag and diffusion coefficients of heavy quarks in the pre-hydrodynamic quantum chromodynamic (QCD) plasma with the state-of-the-art QCD effective kinetic theory (EKT) solver. We present the time, momentum, an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2306.02530","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2306.02530/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":"2306.02530","created_at":"2026-07-05T07:21:11.218271+00:00"},{"alias_kind":"arxiv_version","alias_value":"2306.02530v2","created_at":"2026-07-05T07:21:11.218271+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2306.02530","created_at":"2026-07-05T07:21:11.218271+00:00"},{"alias_kind":"pith_short_12","alias_value":"WSAUKK3RH7F2","created_at":"2026-07-05T07:21:11.218271+00:00"},{"alias_kind":"pith_short_16","alias_value":"WSAUKK3RH7F2UC2B","created_at":"2026-07-05T07:21:11.218271+00:00"},{"alias_kind":"pith_short_8","alias_value":"WSAUKK3R","created_at":"2026-07-05T07:21:11.218271+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07796","citing_title":"Azimuthal momentum isotropization in the Quark-Gluon Plasma thermalization","ref_index":24,"is_internal_anchor":true},{"citing_arxiv_id":"2606.13646","citing_title":"Observable Dependence of Viscous Corrections in QGP: Heavy Quarks and Dileptons in Chapman--Enskog Theory","ref_index":36,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08520","citing_title":"Kinetic and canonical momentum broadening in the Glasma","ref_index":69,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WSAUKK3RH7F2UC2BW4I2AEGJTB","json":"https://pith.science/pith/WSAUKK3RH7F2UC2BW4I2AEGJTB.json","graph_json":"https://pith.science/api/pith-number/WSAUKK3RH7F2UC2BW4I2AEGJTB/graph.json","events_json":"https://pith.science/api/pith-number/WSAUKK3RH7F2UC2BW4I2AEGJTB/events.json","paper":"https://pith.science/paper/WSAUKK3R"},"agent_actions":{"view_html":"https://pith.science/pith/WSAUKK3RH7F2UC2BW4I2AEGJTB","download_json":"https://pith.science/pith/WSAUKK3RH7F2UC2BW4I2AEGJTB.json","view_paper":"https://pith.science/paper/WSAUKK3R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2306.02530&json=true","fetch_graph":"https://pith.science/api/pith-number/WSAUKK3RH7F2UC2BW4I2AEGJTB/graph.json","fetch_events":"https://pith.science/api/pith-number/WSAUKK3RH7F2UC2BW4I2AEGJTB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WSAUKK3RH7F2UC2BW4I2AEGJTB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WSAUKK3RH7F2UC2BW4I2AEGJTB/action/storage_attestation","attest_author":"https://pith.science/pith/WSAUKK3RH7F2UC2BW4I2AEGJTB/action/author_attestation","sign_citation":"https://pith.science/pith/WSAUKK3RH7F2UC2BW4I2AEGJTB/action/citation_signature","submit_replication":"https://pith.science/pith/WSAUKK3RH7F2UC2BW4I2AEGJTB/action/replication_record"}},"created_at":"2026-07-05T07:21:11.218271+00:00","updated_at":"2026-07-05T07:21:11.218271+00:00"}