{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:GDYGTFOFFOXFJB7R5TPWRRWIZE","short_pith_number":"pith:GDYGTFOF","schema_version":"1.0","canonical_sha256":"30f06995c52bae5487f1ecdf68c6c8c9351649474bfae63c565bdac9358ba2c3","source":{"kind":"arxiv","id":"1812.11310","version":2},"attestation_state":"computed","paper":{"title":"Magneto-transport in an anomalous fluid with weakly broken symmetries, in weak and strong regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","nucl-th"],"primary_cat":"hep-th","authors_text":"Armin Ghazi, Farid Taghinavaz, Navid Abbasi, Omid Tavakol","submitted_at":"2018-12-29T08:12:48Z","abstract_excerpt":"We consider a general system with weakly broken time and translation symmetries. We assume the system also possesses a $U(1)$ symmetry which is not only weakly broken, but is anomalous. We use the second order chiral quasi-hydrodynamics to compute the magneto-conductivities in the system in the presence of a weak magnetic field. Analogous to electrical and thermoelectric conductivities, it turns out that the thermal conductivity is identified with a coefficient which depends on the mixed gauge-gravitational anomaly. By applying our general formulas to a free system of Weyl fermions at low temp"},"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":"1812.11310","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-29T08:12:48Z","cross_cats_sorted":["cond-mat.str-el","nucl-th"],"title_canon_sha256":"f79ae73696598777d86f1c22ed0f72a64b88e13766400921b58228d4d4ff104f","abstract_canon_sha256":"08a56ad9c87319d8c1e22624db271908981f9044b904d417ee56e35c587c1505"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:42:25.264550Z","signature_b64":"eVtdfimasVpO7PpM6Gy1F5qlsV227vJwCzl8Uu/cnJierwcxMK6WiNrKSgjI+8/G2iziwFYV9Uzj4X8RGhxKCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"30f06995c52bae5487f1ecdf68c6c8c9351649474bfae63c565bdac9358ba2c3","last_reissued_at":"2026-05-17T23:42:25.263832Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:42:25.263832Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magneto-transport in an anomalous fluid with weakly broken symmetries, in weak and strong regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","nucl-th"],"primary_cat":"hep-th","authors_text":"Armin Ghazi, Farid Taghinavaz, Navid Abbasi, Omid Tavakol","submitted_at":"2018-12-29T08:12:48Z","abstract_excerpt":"We consider a general system with weakly broken time and translation symmetries. We assume the system also possesses a $U(1)$ symmetry which is not only weakly broken, but is anomalous. We use the second order chiral quasi-hydrodynamics to compute the magneto-conductivities in the system in the presence of a weak magnetic field. Analogous to electrical and thermoelectric conductivities, it turns out that the thermal conductivity is identified with a coefficient which depends on the mixed gauge-gravitational anomaly. By applying our general formulas to a free system of Weyl fermions at low temp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.11310","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":""},"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":"1812.11310","created_at":"2026-05-17T23:42:25.263944+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.11310v2","created_at":"2026-05-17T23:42:25.263944+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.11310","created_at":"2026-05-17T23:42:25.263944+00:00"},{"alias_kind":"pith_short_12","alias_value":"GDYGTFOFFOXF","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_16","alias_value":"GDYGTFOFFOXFJB7R","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_8","alias_value":"GDYGTFOF","created_at":"2026-05-18T12:32:25.280505+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/GDYGTFOFFOXFJB7R5TPWRRWIZE","json":"https://pith.science/pith/GDYGTFOFFOXFJB7R5TPWRRWIZE.json","graph_json":"https://pith.science/api/pith-number/GDYGTFOFFOXFJB7R5TPWRRWIZE/graph.json","events_json":"https://pith.science/api/pith-number/GDYGTFOFFOXFJB7R5TPWRRWIZE/events.json","paper":"https://pith.science/paper/GDYGTFOF"},"agent_actions":{"view_html":"https://pith.science/pith/GDYGTFOFFOXFJB7R5TPWRRWIZE","download_json":"https://pith.science/pith/GDYGTFOFFOXFJB7R5TPWRRWIZE.json","view_paper":"https://pith.science/paper/GDYGTFOF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.11310&json=true","fetch_graph":"https://pith.science/api/pith-number/GDYGTFOFFOXFJB7R5TPWRRWIZE/graph.json","fetch_events":"https://pith.science/api/pith-number/GDYGTFOFFOXFJB7R5TPWRRWIZE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GDYGTFOFFOXFJB7R5TPWRRWIZE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GDYGTFOFFOXFJB7R5TPWRRWIZE/action/storage_attestation","attest_author":"https://pith.science/pith/GDYGTFOFFOXFJB7R5TPWRRWIZE/action/author_attestation","sign_citation":"https://pith.science/pith/GDYGTFOFFOXFJB7R5TPWRRWIZE/action/citation_signature","submit_replication":"https://pith.science/pith/GDYGTFOFFOXFJB7R5TPWRRWIZE/action/replication_record"}},"created_at":"2026-05-17T23:42:25.263944+00:00","updated_at":"2026-05-17T23:42:25.263944+00:00"}