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Since the standard gauge fixing and ghost analysis applies to this theory, the ghost contribution to the chiral anomaly is $-1$ times the standard chiral anomaly for spin-$\\frac{1}{2}$. Calculation of the fermion loop Feynman diagrams contributing to the coupled model anomaly gives a result of $6$ times the standard anomaly, so the total anomaly is $5$"},"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":"1903.06189","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-03-14T18:02:32Z","cross_cats_sorted":[],"title_canon_sha256":"eb9ad9487a6f3edba22dcca8f44d1a8735990199fc613b31ffd394019f333f4c","abstract_canon_sha256":"2020e583f32d247312a161b2399d4efb835d3abe38b07ad95d7c9513f1fd38a6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:44:11.740065Z","signature_b64":"sGBRVXXq03JIYb+Zrwpb7kHVaSpv00D159jBLeZVKcDzFo20Q/S2dBKCMuNyzDE3hbjXTUkz73XbhNAYXj6hDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d15085f9905d8c1d774f64187fabb79322e95c6f422989bc4a6a7588456e5aa","last_reissued_at":"2026-05-17T23:44:11.739380Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:44:11.739380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chiral Anomaly Calculation in the Extended Coupled Rarita-Schwinger Mode","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Pablo Pais, Stephen L. 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