{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:P3YD5WXVHJLLMMGEZGSFKFZ22M","short_pith_number":"pith:P3YD5WXV","canonical_record":{"source":{"id":"nucl-th/0111040","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2001-11-13T15:20:57Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"133ee066a63f964bcf620391a99fb34d4b9bdbde6b0e574a84b0e92034daa59c","abstract_canon_sha256":"d46e46ad963153831e2843f7c38ee175c8b6f421298ef53c25f74f790ca86fa4"},"schema_version":"1.0"},"canonical_sha256":"7ef03edaf53a56b630c4c9a455173ad33c4124204a8cd3de9ea092e49bbdb48c","source":{"kind":"arxiv","id":"nucl-th/0111040","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0111040","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0111040v2","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0111040","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"pith_short_12","alias_value":"P3YD5WXVHJLL","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"pith_short_16","alias_value":"P3YD5WXVHJLLMMGE","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"pith_short_8","alias_value":"P3YD5WXV","created_at":"2026-07-04T15:32:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:P3YD5WXVHJLLMMGEZGSFKFZ22M","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/0111040","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2001-11-13T15:20:57Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"133ee066a63f964bcf620391a99fb34d4b9bdbde6b0e574a84b0e92034daa59c","abstract_canon_sha256":"d46e46ad963153831e2843f7c38ee175c8b6f421298ef53c25f74f790ca86fa4"},"schema_version":"1.0"},"canonical_sha256":"7ef03edaf53a56b630c4c9a455173ad33c4124204a8cd3de9ea092e49bbdb48c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:32:34.979602Z","signature_b64":"trMSNRsjK2NILRLerF8bQIniQAIh7dxXFznCV2HuMJLYFaWoEwepZPLSUfC9JbVCNBQYNnA2bwzf8fvDHwEmCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ef03edaf53a56b630c4c9a455173ad33c4124204a8cd3de9ea092e49bbdb48c","last_reissued_at":"2026-07-04T15:32:34.977724Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:32:34.977724Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/0111040","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:32:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RfMKF8/saCPqBf2jrsSu+usm3yOaTQ8uB8UIx3yTHB1U2o/gGdHBeap4eA2g/oS8KzUFIa6Z12dGyOqiprQjBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T07:36:25.445389Z"},"content_sha256":"397cc48166c9e13315d27c42a30e8dc56345c509edcba4f22f36ecc58baab756","schema_version":"1.0","event_id":"sha256:397cc48166c9e13315d27c42a30e8dc56345c509edcba4f22f36ecc58baab756"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:P3YD5WXVHJLLMMGEZGSFKFZ22M","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Kinetic Equation for Gluons in the Background Gauge of QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"H. St\\\"ocker, K. Redlich, Q. Wang, W. Greiner","submitted_at":"2001-11-13T15:20:57Z","abstract_excerpt":"We derive the quantum kinetic equation for a pure gluon plasma, applying the background field and closed-time-path method. The derivation is more general and transparent than earlier works. A term in the equation is found which, as in the classical case, corresponds to the color charge precession for partons moving in the gauge field."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0111040","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/nucl-th/0111040/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:32:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QmcB8MirEU6BQvXyGDO2SoRwIFHueuVtEU5jNOX9ozUna6d58F3R1na98wcdL7Gj8Ov+PluxEfhjukpF8aVvCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T07:36:25.445870Z"},"content_sha256":"1eb25d42e1124260137d2b4cb51f2d7beab12c491163a413e567080fabfea673","schema_version":"1.0","event_id":"sha256:1eb25d42e1124260137d2b4cb51f2d7beab12c491163a413e567080fabfea673"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/P3YD5WXVHJLLMMGEZGSFKFZ22M/bundle.json","state_url":"https://pith.science/pith/P3YD5WXVHJLLMMGEZGSFKFZ22M/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/P3YD5WXVHJLLMMGEZGSFKFZ22M/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-05T07:36:25Z","links":{"resolver":"https://pith.science/pith/P3YD5WXVHJLLMMGEZGSFKFZ22M","bundle":"https://pith.science/pith/P3YD5WXVHJLLMMGEZGSFKFZ22M/bundle.json","state":"https://pith.science/pith/P3YD5WXVHJLLMMGEZGSFKFZ22M/state.json","well_known_bundle":"https://pith.science/.well-known/pith/P3YD5WXVHJLLMMGEZGSFKFZ22M/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:P3YD5WXVHJLLMMGEZGSFKFZ22M","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"d46e46ad963153831e2843f7c38ee175c8b6f421298ef53c25f74f790ca86fa4","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"2001-11-13T15:20:57Z","title_canon_sha256":"133ee066a63f964bcf620391a99fb34d4b9bdbde6b0e574a84b0e92034daa59c"},"schema_version":"1.0","source":{"id":"nucl-th/0111040","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0111040","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0111040v2","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0111040","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"pith_short_12","alias_value":"P3YD5WXVHJLL","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"pith_short_16","alias_value":"P3YD5WXVHJLLMMGE","created_at":"2026-07-04T15:32:34Z"},{"alias_kind":"pith_short_8","alias_value":"P3YD5WXV","created_at":"2026-07-04T15:32:34Z"}],"graph_snapshots":[{"event_id":"sha256:1eb25d42e1124260137d2b4cb51f2d7beab12c491163a413e567080fabfea673","target":"graph","created_at":"2026-07-04T15:32:34Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/nucl-th/0111040/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We derive the quantum kinetic equation for a pure gluon plasma, applying the background field and closed-time-path method. The derivation is more general and transparent than earlier works. A term in the equation is found which, as in the classical case, corresponds to the color charge precession for partons moving in the gauge field.","authors_text":"H. St\\\"ocker, K. Redlich, Q. Wang, W. Greiner","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"2001-11-13T15:20:57Z","title":"Kinetic Equation for Gluons in the Background Gauge of QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0111040","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:397cc48166c9e13315d27c42a30e8dc56345c509edcba4f22f36ecc58baab756","target":"record","created_at":"2026-07-04T15:32:34Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"d46e46ad963153831e2843f7c38ee175c8b6f421298ef53c25f74f790ca86fa4","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"2001-11-13T15:20:57Z","title_canon_sha256":"133ee066a63f964bcf620391a99fb34d4b9bdbde6b0e574a84b0e92034daa59c"},"schema_version":"1.0","source":{"id":"nucl-th/0111040","kind":"arxiv","version":2}},"canonical_sha256":"7ef03edaf53a56b630c4c9a455173ad33c4124204a8cd3de9ea092e49bbdb48c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7ef03edaf53a56b630c4c9a455173ad33c4124204a8cd3de9ea092e49bbdb48c","first_computed_at":"2026-07-04T15:32:34.977724Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:32:34.977724Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"trMSNRsjK2NILRLerF8bQIniQAIh7dxXFznCV2HuMJLYFaWoEwepZPLSUfC9JbVCNBQYNnA2bwzf8fvDHwEmCA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:32:34.979602Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/0111040","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:397cc48166c9e13315d27c42a30e8dc56345c509edcba4f22f36ecc58baab756","sha256:1eb25d42e1124260137d2b4cb51f2d7beab12c491163a413e567080fabfea673"],"state_sha256":"bb8d5b8da98693f46ebc18b84ba54d54d2612d1e57742eb454ca76d936cf23e7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1ZzpTr/poQg2r1ajmQ/j3AZkRURgiMvbF/yU/w+RCahd/w5jFnZuaYdxNnjIQcSbbp8wzaRnezBMrmLhcTqUCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T07:36:25.449830Z","bundle_sha256":"44ad49f9d5e26ff2290ba990d7011b192aab038e5d3703567e22ed75ca046ed4"}}