{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:MR63HQD3KMJPECE2UVBTYQVLTV","short_pith_number":"pith:MR63HQD3","schema_version":"1.0","canonical_sha256":"647db3c07b5312f2089aa5433c42ab9d50b86b34fabd414c9336c27ec7b3a4e0","source":{"kind":"arxiv","id":"1207.5824","version":1},"attestation_state":"computed","paper":{"title":"Thermodynamics, gravitational anomalies and cones","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-ph"],"primary_cat":"hep-th","authors_text":"Amos Yarom, Kristan Jensen, R. Loganayagam","submitted_at":"2012-07-24T20:54:10Z","abstract_excerpt":"By studying the Euclidean partition function on a cone, we argue that pure and mixed gravitational anomalies generate a \"Casimir momentum\" which manifests itself as parity violating coefficients in the hydrodynamic stress tensor and charge current. The coefficients generated by these anomalies enter at a lower order in the hydrodynamic gradient expansion than would be naively expected. In 1+1 dimensions, the gravitational anomaly affects coefficients at zeroth order in the gradient expansion. The mixed anomaly in 3+1 dimensions controls the value of coefficients at first order in the gradient "},"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":"1207.5824","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-24T20:54:10Z","cross_cats_sorted":["cond-mat.str-el","hep-ph"],"title_canon_sha256":"126d73386ab98609f7425b81ef24eb4c114407db0f3da6396012d21919cc7d7e","abstract_canon_sha256":"f15b1d0107109b28e000d49192078a9972611b6e83d45e0acfed58d7d1c8d686"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:06:13.720523Z","signature_b64":"eUQuq9Xlljo+xW9/2m8qT0hwjzGN465W9h+IrTI6GK08DRNzd1leDWFW6wn6BajJUQDZvQHLcy2ogZZETZUJDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"647db3c07b5312f2089aa5433c42ab9d50b86b34fabd414c9336c27ec7b3a4e0","last_reissued_at":"2026-05-18T03:06:13.720082Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:06:13.720082Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamics, gravitational anomalies and cones","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-ph"],"primary_cat":"hep-th","authors_text":"Amos Yarom, Kristan Jensen, R. Loganayagam","submitted_at":"2012-07-24T20:54:10Z","abstract_excerpt":"By studying the Euclidean partition function on a cone, we argue that pure and mixed gravitational anomalies generate a \"Casimir momentum\" which manifests itself as parity violating coefficients in the hydrodynamic stress tensor and charge current. The coefficients generated by these anomalies enter at a lower order in the hydrodynamic gradient expansion than would be naively expected. In 1+1 dimensions, the gravitational anomaly affects coefficients at zeroth order in the gradient expansion. The mixed anomaly in 3+1 dimensions controls the value of coefficients at first order in the gradient "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.5824","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":"1207.5824","created_at":"2026-05-18T03:06:13.720151+00:00"},{"alias_kind":"arxiv_version","alias_value":"1207.5824v1","created_at":"2026-05-18T03:06:13.720151+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.5824","created_at":"2026-05-18T03:06:13.720151+00:00"},{"alias_kind":"pith_short_12","alias_value":"MR63HQD3KMJP","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_16","alias_value":"MR63HQD3KMJPECE2","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_8","alias_value":"MR63HQD3","created_at":"2026-05-18T12:27:14.488303+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/MR63HQD3KMJPECE2UVBTYQVLTV","json":"https://pith.science/pith/MR63HQD3KMJPECE2UVBTYQVLTV.json","graph_json":"https://pith.science/api/pith-number/MR63HQD3KMJPECE2UVBTYQVLTV/graph.json","events_json":"https://pith.science/api/pith-number/MR63HQD3KMJPECE2UVBTYQVLTV/events.json","paper":"https://pith.science/paper/MR63HQD3"},"agent_actions":{"view_html":"https://pith.science/pith/MR63HQD3KMJPECE2UVBTYQVLTV","download_json":"https://pith.science/pith/MR63HQD3KMJPECE2UVBTYQVLTV.json","view_paper":"https://pith.science/paper/MR63HQD3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1207.5824&json=true","fetch_graph":"https://pith.science/api/pith-number/MR63HQD3KMJPECE2UVBTYQVLTV/graph.json","fetch_events":"https://pith.science/api/pith-number/MR63HQD3KMJPECE2UVBTYQVLTV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MR63HQD3KMJPECE2UVBTYQVLTV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MR63HQD3KMJPECE2UVBTYQVLTV/action/storage_attestation","attest_author":"https://pith.science/pith/MR63HQD3KMJPECE2UVBTYQVLTV/action/author_attestation","sign_citation":"https://pith.science/pith/MR63HQD3KMJPECE2UVBTYQVLTV/action/citation_signature","submit_replication":"https://pith.science/pith/MR63HQD3KMJPECE2UVBTYQVLTV/action/replication_record"}},"created_at":"2026-05-18T03:06:13.720151+00:00","updated_at":"2026-05-18T03:06:13.720151+00:00"}