{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:F3L5DQ3XPLEU2TLHSBH4TKTKVC","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":"fee958f6ba78503608d3eef23a7a8f27c82299fd5093a0999f6da0b541c88b3b","cross_cats_sorted":["hep-ph","math-ph","math.MP","physics.flu-dyn"],"license":"","primary_cat":"hep-th","submitted_at":"2002-10-15T19:50:06Z","title_canon_sha256":"77fccbfcc8c0109d00c2aa73072a616062ea5896f3b56cab21460bca813f2463"},"schema_version":"1.0","source":{"id":"hep-th/0210143","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0210143","created_at":"2026-07-04T16:34:55Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0210143v2","created_at":"2026-07-04T16:34:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0210143","created_at":"2026-07-04T16:34:55Z"},{"alias_kind":"pith_short_12","alias_value":"F3L5DQ3XPLEU","created_at":"2026-07-04T16:34:55Z"},{"alias_kind":"pith_short_16","alias_value":"F3L5DQ3XPLEU2TLH","created_at":"2026-07-04T16:34:55Z"},{"alias_kind":"pith_short_8","alias_value":"F3L5DQ3X","created_at":"2026-07-04T16:34:55Z"}],"graph_snapshots":[{"event_id":"sha256:ee2efd82f393079254437f24f2cc4d2fe6b074a1ef207b830fb4d190741ef7a9","target":"graph","created_at":"2026-07-04T16:34:55Z","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/hep-th/0210143/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Non-Abelian extensions of fluid dynamics, which can have applications to the quark-gluon plasma, are given. These theories are presented in a symplectic/Lagrangian formulation and involve a fluid generalization of the Kirillov-Kostant form well known in Lie group theory. In our simplest model the fluid flows with velocity v and in presence of non-Abelian chromoelectric/magnetic E^a / B^a fields, the fluid feels a Lorentz force of the form Q_a E^a + (v / c) \\times Q_a B^a, where Q_a is a space-time local non-Abelian charge satisfying a fluid Wong equation [ (D_t + v \\cdot D) Q ]_a = 0 with gaug","authors_text":"B. Bistrovic, H. Li, R. Jackiw, S.-Y. Pi, V.P. Nair","cross_cats":["hep-ph","math-ph","math.MP","physics.flu-dyn"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2002-10-15T19:50:06Z","title":"Non-Abelian Fluid Dynamics in Lagrangian Formulation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0210143","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":"sha256:74d4173c2b396ebe215d42faa4b812eaa940b06c3b518af8964d3a0afd278128","target":"record","created_at":"2026-07-04T16:34:55Z","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":"fee958f6ba78503608d3eef23a7a8f27c82299fd5093a0999f6da0b541c88b3b","cross_cats_sorted":["hep-ph","math-ph","math.MP","physics.flu-dyn"],"license":"","primary_cat":"hep-th","submitted_at":"2002-10-15T19:50:06Z","title_canon_sha256":"77fccbfcc8c0109d00c2aa73072a616062ea5896f3b56cab21460bca813f2463"},"schema_version":"1.0","source":{"id":"hep-th/0210143","kind":"arxiv","version":2}},"canonical_sha256":"2ed7d1c3777ac94d4d67904fc9aa6aa8bc501b675702410f25b3c5e5bb1a156f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2ed7d1c3777ac94d4d67904fc9aa6aa8bc501b675702410f25b3c5e5bb1a156f","first_computed_at":"2026-07-04T16:34:55.971121Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:34:55.971121Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4qfNMI03e/uP8ANrb/hzU93HmLKUsIMuj2S7BndbiPnHKBjBM0kiaVBiV8Xxh2HEzLOQVxFcqbhs8Cxak4ZUCw==","signature_status":"signed_v1","signed_at":"2026-07-04T16:34:55.971535Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0210143","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:74d4173c2b396ebe215d42faa4b812eaa940b06c3b518af8964d3a0afd278128","sha256:ee2efd82f393079254437f24f2cc4d2fe6b074a1ef207b830fb4d190741ef7a9"],"state_sha256":"98888a89f79e3cd85c16988cd5c9ceb53fbcbff295d4ebbed540848fbb39a613"}