{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:FEKEABHTL5UEXCWTDJHCCDDET6","short_pith_number":"pith:FEKEABHT","canonical_record":{"source":{"id":"1807.07608","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-19T19:00:17Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"912abbf392eb53a46a32dfc76cf7a80bf86f5295f0b0fb5cd642b4e9ec18f60e","abstract_canon_sha256":"16eedafe6c2f390a4a6df79a3e1e82455694179615414ab7e5758a0b12a48ef3"},"schema_version":"1.0"},"canonical_sha256":"29144004f35f684b8ad31a4e210c649f9fcb218a33cc3faf47055ecd8140fe64","source":{"kind":"arxiv","id":"1807.07608","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.07608","created_at":"2026-05-17T23:54:43Z"},{"alias_kind":"arxiv_version","alias_value":"1807.07608v3","created_at":"2026-05-17T23:54:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.07608","created_at":"2026-05-17T23:54:43Z"},{"alias_kind":"pith_short_12","alias_value":"FEKEABHTL5UE","created_at":"2026-05-18T12:32:22Z"},{"alias_kind":"pith_short_16","alias_value":"FEKEABHTL5UEXCWT","created_at":"2026-05-18T12:32:22Z"},{"alias_kind":"pith_short_8","alias_value":"FEKEABHT","created_at":"2026-05-18T12:32:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:FEKEABHTL5UEXCWTDJHCCDDET6","target":"record","payload":{"canonical_record":{"source":{"id":"1807.07608","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-19T19:00:17Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"912abbf392eb53a46a32dfc76cf7a80bf86f5295f0b0fb5cd642b4e9ec18f60e","abstract_canon_sha256":"16eedafe6c2f390a4a6df79a3e1e82455694179615414ab7e5758a0b12a48ef3"},"schema_version":"1.0"},"canonical_sha256":"29144004f35f684b8ad31a4e210c649f9fcb218a33cc3faf47055ecd8140fe64","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:54:43.794303Z","signature_b64":"k0ASwVZzfWG6OyuxZ4PtADLGEOFGsWkZtf8O1sBDK7Qqff+2uTiT6EhzaJCK7ZLXjlaQndkks+OqeCjNytmjCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"29144004f35f684b8ad31a4e210c649f9fcb218a33cc3faf47055ecd8140fe64","last_reissued_at":"2026-05-17T23:54:43.793657Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:54:43.793657Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1807.07608","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:54:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KnrmPSOxOiIRCM2b0aOxXLOICV79g3/H/LY9uindB5eYPCSbgBmz+9yuSPW5inHeLa84WT1XoCXxjg1Z0Mx0Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T00:58:21.239515Z"},"content_sha256":"b8d500154c8f9ba9b0ee291b4d3b776cfb3ef3ab3f98f55dcbae7840717202a7","schema_version":"1.0","event_id":"sha256:b8d500154c8f9ba9b0ee291b4d3b776cfb3ef3ab3f98f55dcbae7840717202a7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:FEKEABHTL5UEXCWTDJHCCDDET6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Hydrodynamic modes in a magnetized chiral plasma with vorticity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"D. O. Rybalka, E. V. Gorbar, I. A. Shovkovy","submitted_at":"2018-07-19T19:00:17Z","abstract_excerpt":"By making use of a covariant formulation of the chiral kinetic theory in the relaxation-time approximation, we derive the first-order dissipative hydrodynamics equations for a charged chiral plasma with background electromagnetic fields. We identify the global equilibrium state for a rotating chiral plasma confined to a cylindrical region with realistic boundary conditions. Then, by using linearized hydrodynamic equations, supplemented by the Maxwell equations, we study hydrodynamic modes of magnetized rotating chiral plasma in the regimes of high temperature and high density. We find that, in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.07608","kind":"arxiv","version":3},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:54:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wlHhN+0uLmKYI3UGfUPhpf5Ikgwj80bMgh++xo4y1vVxOOuVgU3Vybu0U8OvYEJv3CdIE0Ubj+Vlz4EN4402CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T00:58:21.239985Z"},"content_sha256":"fce4a78d8c5732881c4307d45b379748c749500939d294a4944999f4fdad998d","schema_version":"1.0","event_id":"sha256:fce4a78d8c5732881c4307d45b379748c749500939d294a4944999f4fdad998d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FEKEABHTL5UEXCWTDJHCCDDET6/bundle.json","state_url":"https://pith.science/pith/FEKEABHTL5UEXCWTDJHCCDDET6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FEKEABHTL5UEXCWTDJHCCDDET6/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":"2026-08-04T00:58:21Z","links":{"resolver":"https://pith.science/pith/FEKEABHTL5UEXCWTDJHCCDDET6","bundle":"https://pith.science/pith/FEKEABHTL5UEXCWTDJHCCDDET6/bundle.json","state":"https://pith.science/pith/FEKEABHTL5UEXCWTDJHCCDDET6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FEKEABHTL5UEXCWTDJHCCDDET6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:FEKEABHTL5UEXCWTDJHCCDDET6","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":"16eedafe6c2f390a4a6df79a3e1e82455694179615414ab7e5758a0b12a48ef3","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-19T19:00:17Z","title_canon_sha256":"912abbf392eb53a46a32dfc76cf7a80bf86f5295f0b0fb5cd642b4e9ec18f60e"},"schema_version":"1.0","source":{"id":"1807.07608","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.07608","created_at":"2026-05-17T23:54:43Z"},{"alias_kind":"arxiv_version","alias_value":"1807.07608v3","created_at":"2026-05-17T23:54:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.07608","created_at":"2026-05-17T23:54:43Z"},{"alias_kind":"pith_short_12","alias_value":"FEKEABHTL5UE","created_at":"2026-05-18T12:32:22Z"},{"alias_kind":"pith_short_16","alias_value":"FEKEABHTL5UEXCWT","created_at":"2026-05-18T12:32:22Z"},{"alias_kind":"pith_short_8","alias_value":"FEKEABHT","created_at":"2026-05-18T12:32:22Z"}],"graph_snapshots":[{"event_id":"sha256:fce4a78d8c5732881c4307d45b379748c749500939d294a4944999f4fdad998d","target":"graph","created_at":"2026-05-17T23:54:43Z","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"},"paper":{"abstract_excerpt":"By making use of a covariant formulation of the chiral kinetic theory in the relaxation-time approximation, we derive the first-order dissipative hydrodynamics equations for a charged chiral plasma with background electromagnetic fields. We identify the global equilibrium state for a rotating chiral plasma confined to a cylindrical region with realistic boundary conditions. Then, by using linearized hydrodynamic equations, supplemented by the Maxwell equations, we study hydrodynamic modes of magnetized rotating chiral plasma in the regimes of high temperature and high density. We find that, in","authors_text":"D. O. Rybalka, E. V. Gorbar, I. A. Shovkovy","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-19T19:00:17Z","title":"Hydrodynamic modes in a magnetized chiral plasma with vorticity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.07608","kind":"arxiv","version":3},"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:b8d500154c8f9ba9b0ee291b4d3b776cfb3ef3ab3f98f55dcbae7840717202a7","target":"record","created_at":"2026-05-17T23:54:43Z","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":"16eedafe6c2f390a4a6df79a3e1e82455694179615414ab7e5758a0b12a48ef3","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-19T19:00:17Z","title_canon_sha256":"912abbf392eb53a46a32dfc76cf7a80bf86f5295f0b0fb5cd642b4e9ec18f60e"},"schema_version":"1.0","source":{"id":"1807.07608","kind":"arxiv","version":3}},"canonical_sha256":"29144004f35f684b8ad31a4e210c649f9fcb218a33cc3faf47055ecd8140fe64","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"29144004f35f684b8ad31a4e210c649f9fcb218a33cc3faf47055ecd8140fe64","first_computed_at":"2026-05-17T23:54:43.793657Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:54:43.793657Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"k0ASwVZzfWG6OyuxZ4PtADLGEOFGsWkZtf8O1sBDK7Qqff+2uTiT6EhzaJCK7ZLXjlaQndkks+OqeCjNytmjCw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:54:43.794303Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.07608","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b8d500154c8f9ba9b0ee291b4d3b776cfb3ef3ab3f98f55dcbae7840717202a7","sha256:fce4a78d8c5732881c4307d45b379748c749500939d294a4944999f4fdad998d"],"state_sha256":"48b75c58cf934bd3ae280178daf6cf6f3634e3e9d60f6f6463abf8261f298e1b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LAK5RM5425yxktXOs/TZkUIcjGjPKGpsG4ihobmjLkpNPvUi/IOHBt1hibKJgYiTzz6JLB34HMnlQrhHcCWCDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T00:58:21.245134Z","bundle_sha256":"79c0dd59836e7e8b974f54fa63ef77cad32b055a75d85f39eb4f2be76ebd81d7"}}