{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:EPDNBKK6T444G3BBIXFZYL2TAR","short_pith_number":"pith:EPDNBKK6","schema_version":"1.0","canonical_sha256":"23c6d0a95e9f39c36c2145cb9c2f530471951f5832736422bff57fd234376199","source":{"kind":"arxiv","id":"1512.02607","version":2},"attestation_state":"computed","paper":{"title":"Global Anomalies and Effective Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"hep-th","authors_text":"Savdeep Sethi, Siavash Golkar","submitted_at":"2015-12-08T19:57:00Z","abstract_excerpt":"We show that matching anomalies under large gauge transformations and large diffeomorphisms can explain the appearance and non-renormalization of couplings in effective field theory. We focus on thermal effective field theory where we argue that the appearance of certain unusual Chern-Simons couplings is a consequence of global anomalies. As an example, we show that a mixed global anomaly in four dimensions fixes the chiral vortical effect coefficient. This is an experimentally measurable prediction from a global anomaly. For certain situations, we propose a simpler method for calculating glob"},"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":"1512.02607","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-12-08T19:57:00Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"75513277b7a2907635eaa7e6bc40fdc51d149ef63d22a360cb3150c5f81e4034","abstract_canon_sha256":"746a97f572f02ff37f804ee5c8ba5f59f14c20425416180b15da0c952caea1b1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:24:23.949562Z","signature_b64":"UQ63uFLp/xcWSW+PTYpcWf0Ry6XrHdsB1/ntFBA3gOOoGM+IFLEgDsW1jJbKE+WrHYX417nYycPwP8BiurCbCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"23c6d0a95e9f39c36c2145cb9c2f530471951f5832736422bff57fd234376199","last_reissued_at":"2026-05-18T01:24:23.948863Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:24:23.948863Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Global Anomalies and Effective Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"hep-th","authors_text":"Savdeep Sethi, Siavash Golkar","submitted_at":"2015-12-08T19:57:00Z","abstract_excerpt":"We show that matching anomalies under large gauge transformations and large diffeomorphisms can explain the appearance and non-renormalization of couplings in effective field theory. We focus on thermal effective field theory where we argue that the appearance of certain unusual Chern-Simons couplings is a consequence of global anomalies. As an example, we show that a mixed global anomaly in four dimensions fixes the chiral vortical effect coefficient. This is an experimentally measurable prediction from a global anomaly. For certain situations, we propose a simpler method for calculating glob"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.02607","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":"1512.02607","created_at":"2026-05-18T01:24:23.948966+00:00"},{"alias_kind":"arxiv_version","alias_value":"1512.02607v2","created_at":"2026-05-18T01:24:23.948966+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.02607","created_at":"2026-05-18T01:24:23.948966+00:00"},{"alias_kind":"pith_short_12","alias_value":"EPDNBKK6T444","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_16","alias_value":"EPDNBKK6T444G3BB","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_8","alias_value":"EPDNBKK6","created_at":"2026-05-18T12:29:19.899920+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/EPDNBKK6T444G3BBIXFZYL2TAR","json":"https://pith.science/pith/EPDNBKK6T444G3BBIXFZYL2TAR.json","graph_json":"https://pith.science/api/pith-number/EPDNBKK6T444G3BBIXFZYL2TAR/graph.json","events_json":"https://pith.science/api/pith-number/EPDNBKK6T444G3BBIXFZYL2TAR/events.json","paper":"https://pith.science/paper/EPDNBKK6"},"agent_actions":{"view_html":"https://pith.science/pith/EPDNBKK6T444G3BBIXFZYL2TAR","download_json":"https://pith.science/pith/EPDNBKK6T444G3BBIXFZYL2TAR.json","view_paper":"https://pith.science/paper/EPDNBKK6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1512.02607&json=true","fetch_graph":"https://pith.science/api/pith-number/EPDNBKK6T444G3BBIXFZYL2TAR/graph.json","fetch_events":"https://pith.science/api/pith-number/EPDNBKK6T444G3BBIXFZYL2TAR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EPDNBKK6T444G3BBIXFZYL2TAR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EPDNBKK6T444G3BBIXFZYL2TAR/action/storage_attestation","attest_author":"https://pith.science/pith/EPDNBKK6T444G3BBIXFZYL2TAR/action/author_attestation","sign_citation":"https://pith.science/pith/EPDNBKK6T444G3BBIXFZYL2TAR/action/citation_signature","submit_replication":"https://pith.science/pith/EPDNBKK6T444G3BBIXFZYL2TAR/action/replication_record"}},"created_at":"2026-05-18T01:24:23.948966+00:00","updated_at":"2026-05-18T01:24:23.948966+00:00"}