{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:ERR5G27XEAOJBTUXJCBYZKD6DZ","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":"39b3ce0a5ce053df3ef828d502ffc6eee5a10c6690c4c6d07d8ec9e2b01d06b1","cross_cats_sorted":["hep-ph","physics.flu-dyn"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2022-03-22T09:05:55Z","title_canon_sha256":"2c667ad94a493c70fd5c132c04d1406ca5f827da4ec5cabd71a91515eca5350e"},"schema_version":"1.0","source":{"id":"2203.11549","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2203.11549","created_at":"2026-07-05T04:53:19Z"},{"alias_kind":"arxiv_version","alias_value":"2203.11549v2","created_at":"2026-07-05T04:53:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2203.11549","created_at":"2026-07-05T04:53:19Z"},{"alias_kind":"pith_short_12","alias_value":"ERR5G27XEAOJ","created_at":"2026-07-05T04:53:19Z"},{"alias_kind":"pith_short_16","alias_value":"ERR5G27XEAOJBTUX","created_at":"2026-07-05T04:53:19Z"},{"alias_kind":"pith_short_8","alias_value":"ERR5G27X","created_at":"2026-07-05T04:53:19Z"}],"graph_snapshots":[{"event_id":"sha256:0c1cdff6e4ef2cff230f6ce0665e6865b7ae2ac98267889c4569c1efdf81a334","target":"graph","created_at":"2026-07-05T04:53:19Z","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/2203.11549/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We derive multicomponent relativistic second-order dissipative fluid dynamics from the Boltzmann equations for a reactive mixture of $N_{\\text{spec}}$ particle species with $N_q$ intrinsic quantum numbers (e.g. electric charge, baryon number, and strangeness) using the method of moments. We obtain the continuity equations for multiple conserved charges as well as the conservation equations for the total energy and momentum in the single-fluid approximation. These $4+N_q$ conservation laws are closed by deriving the second-order equations of motion for the dissipative quantities in the $(10+4N_","authors_text":"Carsten Greiner, Dirk H. Rischke, Etele Moln\\'ar, Harri Niemi, Jan A. Fotakis","cross_cats":["hep-ph","physics.flu-dyn"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2022-03-22T09:05:55Z","title":"Multicomponent relativistic dissipative fluid dynamics from the Boltzmann equation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2203.11549","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:cd05e75d615277b4c7aea0fcd9c3ee6118ec9ef7b732c71bd028e12716ea8a1a","target":"record","created_at":"2026-07-05T04:53:19Z","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":"39b3ce0a5ce053df3ef828d502ffc6eee5a10c6690c4c6d07d8ec9e2b01d06b1","cross_cats_sorted":["hep-ph","physics.flu-dyn"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2022-03-22T09:05:55Z","title_canon_sha256":"2c667ad94a493c70fd5c132c04d1406ca5f827da4ec5cabd71a91515eca5350e"},"schema_version":"1.0","source":{"id":"2203.11549","kind":"arxiv","version":2}},"canonical_sha256":"2463d36bf7201c90ce9748838ca87e1e4fec14f2acd84b1aa81125b7315bb212","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2463d36bf7201c90ce9748838ca87e1e4fec14f2acd84b1aa81125b7315bb212","first_computed_at":"2026-07-05T04:53:19.098745Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:53:19.098745Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hep31WVotieO9jnvAr9qO+1ngHrSLaqFpuBUMYpxSOl4rOcba5Al/7g+xj2hfxoxnKSHJC3WU+Qz1rIG+s9ADw==","signature_status":"signed_v1","signed_at":"2026-07-05T04:53:19.099087Z","signed_message":"canonical_sha256_bytes"},"source_id":"2203.11549","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cd05e75d615277b4c7aea0fcd9c3ee6118ec9ef7b732c71bd028e12716ea8a1a","sha256:0c1cdff6e4ef2cff230f6ce0665e6865b7ae2ac98267889c4569c1efdf81a334"],"state_sha256":"c253820c5c409c16acee867022d7fb77cc598b6b200c368ce68cc45ff886ba8f"}