{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:66QDKWT5IHJ4FJKWLCAAA5HKSJ","short_pith_number":"pith:66QDKWT5","schema_version":"1.0","canonical_sha256":"f7a0355a7d41d3c2a55658800074ea92530ad07b7ee86d41eafbd9329efd5acc","source":{"kind":"arxiv","id":"1611.05920","version":1},"attestation_state":"computed","paper":{"title":"Electromagnetic Duality and Entanglement Anomalies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Aron Wall, Ben Michel, William Donnelly","submitted_at":"2016-11-17T22:14:51Z","abstract_excerpt":"Duality is an indispensable tool for describing the strong-coupling dynamics of gauge theories. However, its actual realization is often quite subtle: quantities such as the partition function can transform covariantly, with degrees of freedom rearranged in a nonlocal fashion. We study this phenomenon in the context of the electromagnetic duality of abelian $p$-forms. A careful calculation of the duality anomaly on an arbitrary $D$-dimensional manifold shows that the effective actions agree exactly in odd $D$, while in even $D$ they differ by a term proportional to the Euler number. Despite th"},"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":"1611.05920","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-11-17T22:14:51Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"29274c4428f98bbedde412e63c71fbb36a5c62891f6b73575ba7632a76ca2b77","abstract_canon_sha256":"ac123e8227e7c21b78b54a437519a772fc6dade9c643898c5a198d8222ed4d36"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:03.958343Z","signature_b64":"7+abo7mEl+L2VnP0dJeG7PzLAL9riLCj6v/WlBNVQ/f3MpXvbusXv47LiT/yzmz3rWEMWH+9u5arIRrM7FbYAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f7a0355a7d41d3c2a55658800074ea92530ad07b7ee86d41eafbd9329efd5acc","last_reissued_at":"2026-05-18T00:38:03.957710Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:03.957710Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetic Duality and Entanglement Anomalies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Aron Wall, Ben Michel, William Donnelly","submitted_at":"2016-11-17T22:14:51Z","abstract_excerpt":"Duality is an indispensable tool for describing the strong-coupling dynamics of gauge theories. However, its actual realization is often quite subtle: quantities such as the partition function can transform covariantly, with degrees of freedom rearranged in a nonlocal fashion. We study this phenomenon in the context of the electromagnetic duality of abelian $p$-forms. A careful calculation of the duality anomaly on an arbitrary $D$-dimensional manifold shows that the effective actions agree exactly in odd $D$, while in even $D$ they differ by a term proportional to the Euler number. Despite th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.05920","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":"1611.05920","created_at":"2026-05-18T00:38:03.957803+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.05920v1","created_at":"2026-05-18T00:38:03.957803+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.05920","created_at":"2026-05-18T00:38:03.957803+00:00"},{"alias_kind":"pith_short_12","alias_value":"66QDKWT5IHJ4","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_16","alias_value":"66QDKWT5IHJ4FJKW","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_8","alias_value":"66QDKWT5","created_at":"2026-05-18T12:30:01.593930+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.21494","citing_title":"Non-relativistic limits of $\\mathcal N=4$ supersymmetric Yang-Mills theory and S-duality","ref_index":40,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/66QDKWT5IHJ4FJKWLCAAA5HKSJ","json":"https://pith.science/pith/66QDKWT5IHJ4FJKWLCAAA5HKSJ.json","graph_json":"https://pith.science/api/pith-number/66QDKWT5IHJ4FJKWLCAAA5HKSJ/graph.json","events_json":"https://pith.science/api/pith-number/66QDKWT5IHJ4FJKWLCAAA5HKSJ/events.json","paper":"https://pith.science/paper/66QDKWT5"},"agent_actions":{"view_html":"https://pith.science/pith/66QDKWT5IHJ4FJKWLCAAA5HKSJ","download_json":"https://pith.science/pith/66QDKWT5IHJ4FJKWLCAAA5HKSJ.json","view_paper":"https://pith.science/paper/66QDKWT5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.05920&json=true","fetch_graph":"https://pith.science/api/pith-number/66QDKWT5IHJ4FJKWLCAAA5HKSJ/graph.json","fetch_events":"https://pith.science/api/pith-number/66QDKWT5IHJ4FJKWLCAAA5HKSJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/66QDKWT5IHJ4FJKWLCAAA5HKSJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/66QDKWT5IHJ4FJKWLCAAA5HKSJ/action/storage_attestation","attest_author":"https://pith.science/pith/66QDKWT5IHJ4FJKWLCAAA5HKSJ/action/author_attestation","sign_citation":"https://pith.science/pith/66QDKWT5IHJ4FJKWLCAAA5HKSJ/action/citation_signature","submit_replication":"https://pith.science/pith/66QDKWT5IHJ4FJKWLCAAA5HKSJ/action/replication_record"}},"created_at":"2026-05-18T00:38:03.957803+00:00","updated_at":"2026-05-18T00:38:03.957803+00:00"}