{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:J2BCULE7SHG2IMPYZRTJ2US6SK","short_pith_number":"pith:J2BCULE7","schema_version":"1.0","canonical_sha256":"4e822a2c9f91cda431f8cc669d525e9291ea17c2d9b2f32161082007b13d85b7","source":{"kind":"arxiv","id":"1508.02396","version":2},"attestation_state":"computed","paper":{"title":"The no-drag frame for anomalous chiral fluid","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","nucl-th"],"primary_cat":"hep-th","authors_text":"Ho-Ung Yee, Mikhail A. Stephanov","submitted_at":"2015-08-10T20:05:23Z","abstract_excerpt":"We show that for an anomalous fluid carrying dissipationless chiral magnetic and/or vortical currents there is a frame in which a stationary obstacle experiences no drag, but energy and charge currents do not vanish, resembling superfluidity. However, unlike ordinary superfluid flow, the anomalous chiral currents do transport entropy in this frame. We show that the second law of thermodynamics completely determines the amounts of these anomalous non-dissipative currents in the \"no-drag frame\" as polynomials in temperature and chemical potential with known anomaly coefficients. These general re"},"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":"1508.02396","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-08-10T20:05:23Z","cross_cats_sorted":["cond-mat.mes-hall","nucl-th"],"title_canon_sha256":"cf00632677be597de09f9af8b5ecd8970ce8532436b03ba307ecaf5208dc2265","abstract_canon_sha256":"6c795f997132d8d5aff307648cf9902d0da11a1dc1cb887f839a5f4c47a8d28a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:09.604206Z","signature_b64":"d7C5jr/hAjj1GfbKdZIIVk/3QmcMpQ3HydO5NalwRfvmiavIOoqGNVhq0dwRdUXXVSWscTrrglr+9iiz7IXjAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e822a2c9f91cda431f8cc669d525e9291ea17c2d9b2f32161082007b13d85b7","last_reissued_at":"2026-05-18T01:18:09.603678Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:09.603678Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The no-drag frame for anomalous chiral fluid","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","nucl-th"],"primary_cat":"hep-th","authors_text":"Ho-Ung Yee, Mikhail A. Stephanov","submitted_at":"2015-08-10T20:05:23Z","abstract_excerpt":"We show that for an anomalous fluid carrying dissipationless chiral magnetic and/or vortical currents there is a frame in which a stationary obstacle experiences no drag, but energy and charge currents do not vanish, resembling superfluidity. However, unlike ordinary superfluid flow, the anomalous chiral currents do transport entropy in this frame. We show that the second law of thermodynamics completely determines the amounts of these anomalous non-dissipative currents in the \"no-drag frame\" as polynomials in temperature and chemical potential with known anomaly coefficients. These general re"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.02396","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":"1508.02396","created_at":"2026-05-18T01:18:09.603756+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.02396v2","created_at":"2026-05-18T01:18:09.603756+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.02396","created_at":"2026-05-18T01:18:09.603756+00:00"},{"alias_kind":"pith_short_12","alias_value":"J2BCULE7SHG2","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_16","alias_value":"J2BCULE7SHG2IMPY","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_8","alias_value":"J2BCULE7","created_at":"2026-05-18T12:29:27.538025+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/J2BCULE7SHG2IMPYZRTJ2US6SK","json":"https://pith.science/pith/J2BCULE7SHG2IMPYZRTJ2US6SK.json","graph_json":"https://pith.science/api/pith-number/J2BCULE7SHG2IMPYZRTJ2US6SK/graph.json","events_json":"https://pith.science/api/pith-number/J2BCULE7SHG2IMPYZRTJ2US6SK/events.json","paper":"https://pith.science/paper/J2BCULE7"},"agent_actions":{"view_html":"https://pith.science/pith/J2BCULE7SHG2IMPYZRTJ2US6SK","download_json":"https://pith.science/pith/J2BCULE7SHG2IMPYZRTJ2US6SK.json","view_paper":"https://pith.science/paper/J2BCULE7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.02396&json=true","fetch_graph":"https://pith.science/api/pith-number/J2BCULE7SHG2IMPYZRTJ2US6SK/graph.json","fetch_events":"https://pith.science/api/pith-number/J2BCULE7SHG2IMPYZRTJ2US6SK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J2BCULE7SHG2IMPYZRTJ2US6SK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J2BCULE7SHG2IMPYZRTJ2US6SK/action/storage_attestation","attest_author":"https://pith.science/pith/J2BCULE7SHG2IMPYZRTJ2US6SK/action/author_attestation","sign_citation":"https://pith.science/pith/J2BCULE7SHG2IMPYZRTJ2US6SK/action/citation_signature","submit_replication":"https://pith.science/pith/J2BCULE7SHG2IMPYZRTJ2US6SK/action/replication_record"}},"created_at":"2026-05-18T01:18:09.603756+00:00","updated_at":"2026-05-18T01:18:09.603756+00:00"}