{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:LSYSWUP4AGV37AJQUUONBZPO6T","short_pith_number":"pith:LSYSWUP4","schema_version":"1.0","canonical_sha256":"5cb12b51fc01abbf8130a51cd0e5eef4f8d96b041fd21e4e1afcdfee969b835a","source":{"kind":"arxiv","id":"1409.8339","version":1},"attestation_state":"computed","paper":{"title":"All-fermion electrodynamics and fermion number anomaly inflow","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Brian Swingle, John McGreevy, S. M. Kravec","submitted_at":"2014-09-29T22:13:36Z","abstract_excerpt":"We demonstrate that 3+1-dimensional quantum electrodynamics with fermionic charges, fermionic monopoles, and fermionic dyons arises at the edge of a 4+1-dimensional gapped state with short-range entanglement. This state cannot be adiabatically connected to a product state, even in the absence of any symmetry. This provides independent evidence for the obstruction found by arXiv:1306.3238 to a 3+1-dimensional short-distance completion of all-fermion electrodynamics. The non-triviality of the bulk is demonstrated by a novel fermion number anomaly."},"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":"1409.8339","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-09-29T22:13:36Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"c7692ed3beff443064cc985aa1d787617afad679cb9ab826bd0709c4a45a733e","abstract_canon_sha256":"5cf020a31f9bd4432ef277bbc1301bef882d9bb8d149303c8d4d6b84aa7a0398"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:29:46.907441Z","signature_b64":"3aCc3WRMN6V1GCZiZzVObTOF1+Y6IfdmWfnnDhV3H8Eg1T55hac5cYNudhRRHq8FwNN5qBJos/8vNltoySAiBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5cb12b51fc01abbf8130a51cd0e5eef4f8d96b041fd21e4e1afcdfee969b835a","last_reissued_at":"2026-05-18T01:29:46.906971Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:29:46.906971Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"All-fermion electrodynamics and fermion number anomaly inflow","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Brian Swingle, John McGreevy, S. M. Kravec","submitted_at":"2014-09-29T22:13:36Z","abstract_excerpt":"We demonstrate that 3+1-dimensional quantum electrodynamics with fermionic charges, fermionic monopoles, and fermionic dyons arises at the edge of a 4+1-dimensional gapped state with short-range entanglement. This state cannot be adiabatically connected to a product state, even in the absence of any symmetry. This provides independent evidence for the obstruction found by arXiv:1306.3238 to a 3+1-dimensional short-distance completion of all-fermion electrodynamics. The non-triviality of the bulk is demonstrated by a novel fermion number anomaly."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.8339","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":"1409.8339","created_at":"2026-05-18T01:29:46.907040+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.8339v1","created_at":"2026-05-18T01:29:46.907040+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.8339","created_at":"2026-05-18T01:29:46.907040+00:00"},{"alias_kind":"pith_short_12","alias_value":"LSYSWUP4AGV3","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_16","alias_value":"LSYSWUP4AGV37AJQ","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_8","alias_value":"LSYSWUP4","created_at":"2026-05-18T12:28:38.356838+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2602.09105","citing_title":"Generalized Families of QFTs","ref_index":33,"is_internal_anchor":true},{"citing_arxiv_id":"2604.08736","citing_title":"Exact SL(2,Z)-Structure of Lattice Maxwell Theory with $\\theta$-term in Modified Villain Formulation","ref_index":40,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LSYSWUP4AGV37AJQUUONBZPO6T","json":"https://pith.science/pith/LSYSWUP4AGV37AJQUUONBZPO6T.json","graph_json":"https://pith.science/api/pith-number/LSYSWUP4AGV37AJQUUONBZPO6T/graph.json","events_json":"https://pith.science/api/pith-number/LSYSWUP4AGV37AJQUUONBZPO6T/events.json","paper":"https://pith.science/paper/LSYSWUP4"},"agent_actions":{"view_html":"https://pith.science/pith/LSYSWUP4AGV37AJQUUONBZPO6T","download_json":"https://pith.science/pith/LSYSWUP4AGV37AJQUUONBZPO6T.json","view_paper":"https://pith.science/paper/LSYSWUP4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.8339&json=true","fetch_graph":"https://pith.science/api/pith-number/LSYSWUP4AGV37AJQUUONBZPO6T/graph.json","fetch_events":"https://pith.science/api/pith-number/LSYSWUP4AGV37AJQUUONBZPO6T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LSYSWUP4AGV37AJQUUONBZPO6T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LSYSWUP4AGV37AJQUUONBZPO6T/action/storage_attestation","attest_author":"https://pith.science/pith/LSYSWUP4AGV37AJQUUONBZPO6T/action/author_attestation","sign_citation":"https://pith.science/pith/LSYSWUP4AGV37AJQUUONBZPO6T/action/citation_signature","submit_replication":"https://pith.science/pith/LSYSWUP4AGV37AJQUUONBZPO6T/action/replication_record"}},"created_at":"2026-05-18T01:29:46.907040+00:00","updated_at":"2026-05-18T01:29:46.907040+00:00"}