{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:4LJRKUJD4O6JJFHPHO7ILDAJ45","short_pith_number":"pith:4LJRKUJD","schema_version":"1.0","canonical_sha256":"e2d3155123e3bc9494ef3bbe858c09e770276bf886f843c611966241891aaf21","source":{"kind":"arxiv","id":"1707.02491","version":1},"attestation_state":"computed","paper":{"title":"Anomalous current from covariant Wigner functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"George Prokhorov, Oleg Teryaev","submitted_at":"2017-07-08T20:23:41Z","abstract_excerpt":"We consider accelerated and rotating media of weakly interacting fermions in local thermodynamic equilibrium. Kinetic properties of this media are described by covariant Wigner function calculated on the basis of relativistic distribution function of particles with spin. We obtain the formulae for axial current beyond the approximation of smallness of thermal vorticity tensor and chemical potential and calculate its divergence. In the massless limit higher order terms in vorticity and chemical potential compensate each other with only the low-order contributions surviving. It is shown, that ax"},"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":"1707.02491","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-08T20:23:41Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"ed3d84917462e40a4eff8d9fb15dd438c30bfccca34752102eea2310142f8832","abstract_canon_sha256":"4893d9c34d570568fcb22bb6405052bb17c2881f5c685c483cbaba2181945be0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:17:09.193247Z","signature_b64":"miKAFMnFTQ0cBQ6bIl/wRnzNte3wpDjwsM2jWy5njqm/MInG3l2i0IcftXOnNkjAtcjHg5ZDRIPbdpfK3cclDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e2d3155123e3bc9494ef3bbe858c09e770276bf886f843c611966241891aaf21","last_reissued_at":"2026-05-18T00:17:09.192768Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:17:09.192768Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomalous current from covariant Wigner functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"George Prokhorov, Oleg Teryaev","submitted_at":"2017-07-08T20:23:41Z","abstract_excerpt":"We consider accelerated and rotating media of weakly interacting fermions in local thermodynamic equilibrium. Kinetic properties of this media are described by covariant Wigner function calculated on the basis of relativistic distribution function of particles with spin. We obtain the formulae for axial current beyond the approximation of smallness of thermal vorticity tensor and chemical potential and calculate its divergence. In the massless limit higher order terms in vorticity and chemical potential compensate each other with only the low-order contributions surviving. It is shown, that ax"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.02491","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":"1707.02491","created_at":"2026-05-18T00:17:09.192850+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.02491v1","created_at":"2026-05-18T00:17:09.192850+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.02491","created_at":"2026-05-18T00:17:09.192850+00:00"},{"alias_kind":"pith_short_12","alias_value":"4LJRKUJD4O6J","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_16","alias_value":"4LJRKUJD4O6JJFHP","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_8","alias_value":"4LJRKUJD","created_at":"2026-05-18T12:31:00.734936+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4LJRKUJD4O6JJFHPHO7ILDAJ45","json":"https://pith.science/pith/4LJRKUJD4O6JJFHPHO7ILDAJ45.json","graph_json":"https://pith.science/api/pith-number/4LJRKUJD4O6JJFHPHO7ILDAJ45/graph.json","events_json":"https://pith.science/api/pith-number/4LJRKUJD4O6JJFHPHO7ILDAJ45/events.json","paper":"https://pith.science/paper/4LJRKUJD"},"agent_actions":{"view_html":"https://pith.science/pith/4LJRKUJD4O6JJFHPHO7ILDAJ45","download_json":"https://pith.science/pith/4LJRKUJD4O6JJFHPHO7ILDAJ45.json","view_paper":"https://pith.science/paper/4LJRKUJD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.02491&json=true","fetch_graph":"https://pith.science/api/pith-number/4LJRKUJD4O6JJFHPHO7ILDAJ45/graph.json","fetch_events":"https://pith.science/api/pith-number/4LJRKUJD4O6JJFHPHO7ILDAJ45/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4LJRKUJD4O6JJFHPHO7ILDAJ45/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4LJRKUJD4O6JJFHPHO7ILDAJ45/action/storage_attestation","attest_author":"https://pith.science/pith/4LJRKUJD4O6JJFHPHO7ILDAJ45/action/author_attestation","sign_citation":"https://pith.science/pith/4LJRKUJD4O6JJFHPHO7ILDAJ45/action/citation_signature","submit_replication":"https://pith.science/pith/4LJRKUJD4O6JJFHPHO7ILDAJ45/action/replication_record"}},"created_at":"2026-05-18T00:17:09.192850+00:00","updated_at":"2026-05-18T00:17:09.192850+00:00"}