{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:OV7OGD2SKS2GEPDOELIS5AW4AX","short_pith_number":"pith:OV7OGD2S","schema_version":"1.0","canonical_sha256":"757ee30f5254b4623c6e22d12e82dc05c6ad348967f69958bdbaed1e1d7dbe7b","source":{"kind":"arxiv","id":"hep-th/9407078","version":2},"attestation_state":"computed","paper":{"title":"Bosonization in Higher Dimensions","license":"","headline":"","cross_cats":["cond-mat","hep-ph"],"primary_cat":"hep-th","authors_text":"C.A. L\\\"utken, C.P. Burgess, F. Quevedo","submitted_at":"1994-07-14T14:39:07Z","abstract_excerpt":"Using the recently discovered connection between bosonization and duality transformations (hep-th/9401105 and hep-th/9403173), we give an explicit path-integral representation for the bosonization of a massive fermion coupled to a U(1) gauge potential (such as electromagnetism) in d space (D=d+1 spacetime) dimensions. The bosonic theory is described by a rank d-1 antisymmetric Kalb-Ramond-type gauge potential. We construct the bosonized lagrangian explicitly in the limit of large fermion mass. We find that the resulting action is local for d=2 (and given by a Chern-Simons action), but nonlocal"},"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":"hep-th/9407078","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-07-14T14:39:07Z","cross_cats_sorted":["cond-mat","hep-ph"],"title_canon_sha256":"e3ecaba3c6b94e9a06d7a3449b5d5f6f223bd246c8e27431c0c244409746aa13","abstract_canon_sha256":"2719e993e6a82238bb1ea881d793bcf5deec0a2acc4f5d9aecbd5fc3d1d4798b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:37.164741Z","signature_b64":"zGMJbHEXXTM0c7Gm5gPjDX8gZKWP9XpLZ4v4jrrATZRxiRSAwbjqWULAr3WNStgMI03KxNWN+JQjzmTc0qjQCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"757ee30f5254b4623c6e22d12e82dc05c6ad348967f69958bdbaed1e1d7dbe7b","last_reissued_at":"2026-05-18T04:15:37.163832Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:37.163832Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bosonization in Higher Dimensions","license":"","headline":"","cross_cats":["cond-mat","hep-ph"],"primary_cat":"hep-th","authors_text":"C.A. L\\\"utken, C.P. Burgess, F. Quevedo","submitted_at":"1994-07-14T14:39:07Z","abstract_excerpt":"Using the recently discovered connection between bosonization and duality transformations (hep-th/9401105 and hep-th/9403173), we give an explicit path-integral representation for the bosonization of a massive fermion coupled to a U(1) gauge potential (such as electromagnetism) in d space (D=d+1 spacetime) dimensions. The bosonic theory is described by a rank d-1 antisymmetric Kalb-Ramond-type gauge potential. We construct the bosonized lagrangian explicitly in the limit of large fermion mass. We find that the resulting action is local for d=2 (and given by a Chern-Simons action), but nonlocal"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9407078","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":"hep-th/9407078","created_at":"2026-05-18T04:15:37.163997+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9407078v2","created_at":"2026-05-18T04:15:37.163997+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9407078","created_at":"2026-05-18T04:15:37.163997+00:00"},{"alias_kind":"pith_short_12","alias_value":"OV7OGD2SKS2G","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"OV7OGD2SKS2GEPDO","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"OV7OGD2S","created_at":"2026-05-18T12:25:47.102015+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/OV7OGD2SKS2GEPDOELIS5AW4AX","json":"https://pith.science/pith/OV7OGD2SKS2GEPDOELIS5AW4AX.json","graph_json":"https://pith.science/api/pith-number/OV7OGD2SKS2GEPDOELIS5AW4AX/graph.json","events_json":"https://pith.science/api/pith-number/OV7OGD2SKS2GEPDOELIS5AW4AX/events.json","paper":"https://pith.science/paper/OV7OGD2S"},"agent_actions":{"view_html":"https://pith.science/pith/OV7OGD2SKS2GEPDOELIS5AW4AX","download_json":"https://pith.science/pith/OV7OGD2SKS2GEPDOELIS5AW4AX.json","view_paper":"https://pith.science/paper/OV7OGD2S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9407078&json=true","fetch_graph":"https://pith.science/api/pith-number/OV7OGD2SKS2GEPDOELIS5AW4AX/graph.json","fetch_events":"https://pith.science/api/pith-number/OV7OGD2SKS2GEPDOELIS5AW4AX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OV7OGD2SKS2GEPDOELIS5AW4AX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OV7OGD2SKS2GEPDOELIS5AW4AX/action/storage_attestation","attest_author":"https://pith.science/pith/OV7OGD2SKS2GEPDOELIS5AW4AX/action/author_attestation","sign_citation":"https://pith.science/pith/OV7OGD2SKS2GEPDOELIS5AW4AX/action/citation_signature","submit_replication":"https://pith.science/pith/OV7OGD2SKS2GEPDOELIS5AW4AX/action/replication_record"}},"created_at":"2026-05-18T04:15:37.163997+00:00","updated_at":"2026-05-18T04:15:37.163997+00:00"}