{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:RAGIBGCDLYH4LQWTOTTDMKFJHW","short_pith_number":"pith:RAGIBGCD","schema_version":"1.0","canonical_sha256":"880c8098435e0fc5c2d374e63628a93d81c8500d0147afc31d5d353dd91b51d7","source":{"kind":"arxiv","id":"2102.06799","version":3},"attestation_state":"computed","paper":{"title":"Boundary electromagnetic duality from homological edge modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math.MP"],"primary_cat":"math-ph","authors_text":"Nicholas J. Teh, Philippe Mathieu","submitted_at":"2021-02-12T22:27:39Z","abstract_excerpt":"Recent years have seen a renewed interest in using `edge modes' to extend the pre-symplectic structure of gauge theory on manifolds with boundaries. Here we further the investigation undertaken in \\cite{FP2018} by using the formalism of homotopy pullback and Deligne-Beilinson cohomology to describe an electromagnetic (EM) duality on the boundary of $M=B^{3}\\times\\mathbb{R}$. Upon breaking a generalized global symmetry, the duality is implemented by a BF-like topological boundary term. We then introduce Wilson line singularities on $\\partial M$ and show that these induce the existence of dual e"},"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":"2102.06799","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2021-02-12T22:27:39Z","cross_cats_sorted":["hep-th","math.MP"],"title_canon_sha256":"73b4151957f3f13bbbb08fcc196d2dec144e9ed3a8da610fe4154a09c2b67d8e","abstract_canon_sha256":"36873673b2f148abd0c7df0256cdde0aef217a536557025c00328088925334b6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:03:18.773169Z","signature_b64":"eSNrhh3VrrV+C1gz03orHydBnoUTfnsyi0f9tJzfqCrAFITUMlLKz7pEmzrkz2msFaXKRrUVlK1X/tkqKfjTAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"880c8098435e0fc5c2d374e63628a93d81c8500d0147afc31d5d353dd91b51d7","last_reissued_at":"2026-07-05T03:03:18.772751Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:03:18.772751Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Boundary electromagnetic duality from homological edge modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math.MP"],"primary_cat":"math-ph","authors_text":"Nicholas J. Teh, Philippe Mathieu","submitted_at":"2021-02-12T22:27:39Z","abstract_excerpt":"Recent years have seen a renewed interest in using `edge modes' to extend the pre-symplectic structure of gauge theory on manifolds with boundaries. Here we further the investigation undertaken in \\cite{FP2018} by using the formalism of homotopy pullback and Deligne-Beilinson cohomology to describe an electromagnetic (EM) duality on the boundary of $M=B^{3}\\times\\mathbb{R}$. Upon breaking a generalized global symmetry, the duality is implemented by a BF-like topological boundary term. We then introduce Wilson line singularities on $\\partial M$ and show that these induce the existence of dual e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2102.06799","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2102.06799/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2102.06799","created_at":"2026-07-05T03:03:18.772806+00:00"},{"alias_kind":"arxiv_version","alias_value":"2102.06799v3","created_at":"2026-07-05T03:03:18.772806+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2102.06799","created_at":"2026-07-05T03:03:18.772806+00:00"},{"alias_kind":"pith_short_12","alias_value":"RAGIBGCDLYH4","created_at":"2026-07-05T03:03:18.772806+00:00"},{"alias_kind":"pith_short_16","alias_value":"RAGIBGCDLYH4LQWT","created_at":"2026-07-05T03:03:18.772806+00:00"},{"alias_kind":"pith_short_8","alias_value":"RAGIBGCD","created_at":"2026-07-05T03:03:18.772806+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.27870","citing_title":"Revisiting boundary electromagnetic duality and edge modes","ref_index":91,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RAGIBGCDLYH4LQWTOTTDMKFJHW","json":"https://pith.science/pith/RAGIBGCDLYH4LQWTOTTDMKFJHW.json","graph_json":"https://pith.science/api/pith-number/RAGIBGCDLYH4LQWTOTTDMKFJHW/graph.json","events_json":"https://pith.science/api/pith-number/RAGIBGCDLYH4LQWTOTTDMKFJHW/events.json","paper":"https://pith.science/paper/RAGIBGCD"},"agent_actions":{"view_html":"https://pith.science/pith/RAGIBGCDLYH4LQWTOTTDMKFJHW","download_json":"https://pith.science/pith/RAGIBGCDLYH4LQWTOTTDMKFJHW.json","view_paper":"https://pith.science/paper/RAGIBGCD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2102.06799&json=true","fetch_graph":"https://pith.science/api/pith-number/RAGIBGCDLYH4LQWTOTTDMKFJHW/graph.json","fetch_events":"https://pith.science/api/pith-number/RAGIBGCDLYH4LQWTOTTDMKFJHW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RAGIBGCDLYH4LQWTOTTDMKFJHW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RAGIBGCDLYH4LQWTOTTDMKFJHW/action/storage_attestation","attest_author":"https://pith.science/pith/RAGIBGCDLYH4LQWTOTTDMKFJHW/action/author_attestation","sign_citation":"https://pith.science/pith/RAGIBGCDLYH4LQWTOTTDMKFJHW/action/citation_signature","submit_replication":"https://pith.science/pith/RAGIBGCDLYH4LQWTOTTDMKFJHW/action/replication_record"}},"created_at":"2026-07-05T03:03:18.772806+00:00","updated_at":"2026-07-05T03:03:18.772806+00:00"}