{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:HNJMDD4QSBB3DP2GP6D2TRWXGL","short_pith_number":"pith:HNJMDD4Q","schema_version":"1.0","canonical_sha256":"3b52c18f909043b1bf467f87a9c6d732c7a2ddbf98fd06f62ac2d64439e083c1","source":{"kind":"arxiv","id":"hep-ph/9406285","version":1},"attestation_state":"computed","paper":{"title":"Classical Transport Theory and Hard Thermal Loops in the Quark-Gluon Plasma","license":"","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"C. Lucchesi, C. Manuel, P.F. Kelly, Q. Liu","submitted_at":"1994-06-10T20:23:53Z","abstract_excerpt":"Classical transport theory for colored particles is investigated and employed to derive the hard thermal loops of QCD. A formal construction of phase-space for color degrees of freedom is presented. The gauge invariance of the non-Abelian Vlasov equations is verified and used as a guiding principle in our approximation scheme.We then derive the generating functional of hard thermal loops from a constraint satisfied at leading-order by the color current. This derivation is more direct than alternative ones based on perturbative quantum field theory, and shows that hard thermal effects in hot QC"},"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/9406285","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-06-10T20:23:53Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"bbce6959e042698ab4deaebe2e754fc996a73e6ad9d5e4a11b796a96d1c31024","abstract_canon_sha256":"baa147afafb7a2b61d30086c5adfe93e1b7bc9c196eee672417353e73741b9a4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:44.083747Z","signature_b64":"fqUrlin4ZWKoQrFBShmBitLYsRwG93+4YKW+z0sYT3zArUcF1JUv3MWIl8ltIQaXOb8yIdcpbiSTFs3CMjLYBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3b52c18f909043b1bf467f87a9c6d732c7a2ddbf98fd06f62ac2d64439e083c1","last_reissued_at":"2026-05-18T04:17:44.083336Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:44.083336Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Classical Transport Theory and Hard Thermal Loops in the Quark-Gluon Plasma","license":"","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"C. Lucchesi, C. Manuel, P.F. Kelly, Q. Liu","submitted_at":"1994-06-10T20:23:53Z","abstract_excerpt":"Classical transport theory for colored particles is investigated and employed to derive the hard thermal loops of QCD. A formal construction of phase-space for color degrees of freedom is presented. The gauge invariance of the non-Abelian Vlasov equations is verified and used as a guiding principle in our approximation scheme.We then derive the generating functional of hard thermal loops from a constraint satisfied at leading-order by the color current. This derivation is more direct than alternative ones based on perturbative quantum field theory, and shows that hard thermal effects in hot QC"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9406285","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/9406285","created_at":"2026-05-18T04:17:44.083406+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9406285v1","created_at":"2026-05-18T04:17:44.083406+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9406285","created_at":"2026-05-18T04:17:44.083406+00:00"},{"alias_kind":"pith_short_12","alias_value":"HNJMDD4QSBB3","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"HNJMDD4QSBB3DP2G","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"HNJMDD4Q","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.22822","citing_title":"Bottom-up open EFT for non-Abelian gauge theory with dynamical color environment","ref_index":24,"is_internal_anchor":true},{"citing_arxiv_id":"2605.10413","citing_title":"Light-front Hamiltonian jet evolution in the Glasma","ref_index":100,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08520","citing_title":"Kinetic and canonical momentum broadening in the Glasma","ref_index":92,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HNJMDD4QSBB3DP2GP6D2TRWXGL","json":"https://pith.science/pith/HNJMDD4QSBB3DP2GP6D2TRWXGL.json","graph_json":"https://pith.science/api/pith-number/HNJMDD4QSBB3DP2GP6D2TRWXGL/graph.json","events_json":"https://pith.science/api/pith-number/HNJMDD4QSBB3DP2GP6D2TRWXGL/events.json","paper":"https://pith.science/paper/HNJMDD4Q"},"agent_actions":{"view_html":"https://pith.science/pith/HNJMDD4QSBB3DP2GP6D2TRWXGL","download_json":"https://pith.science/pith/HNJMDD4QSBB3DP2GP6D2TRWXGL.json","view_paper":"https://pith.science/paper/HNJMDD4Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9406285&json=true","fetch_graph":"https://pith.science/api/pith-number/HNJMDD4QSBB3DP2GP6D2TRWXGL/graph.json","fetch_events":"https://pith.science/api/pith-number/HNJMDD4QSBB3DP2GP6D2TRWXGL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HNJMDD4QSBB3DP2GP6D2TRWXGL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HNJMDD4QSBB3DP2GP6D2TRWXGL/action/storage_attestation","attest_author":"https://pith.science/pith/HNJMDD4QSBB3DP2GP6D2TRWXGL/action/author_attestation","sign_citation":"https://pith.science/pith/HNJMDD4QSBB3DP2GP6D2TRWXGL/action/citation_signature","submit_replication":"https://pith.science/pith/HNJMDD4QSBB3DP2GP6D2TRWXGL/action/replication_record"}},"created_at":"2026-05-18T04:17:44.083406+00:00","updated_at":"2026-05-18T04:17:44.083406+00:00"}