{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:KRKEHUFZP72C2CSZE45UC62JHX","short_pith_number":"pith:KRKEHUFZ","schema_version":"1.0","canonical_sha256":"545443d0b97ff42d0a59273b417b493dea412ecb5bd45fd530f590ca8da6bccd","source":{"kind":"arxiv","id":"1203.5519","version":5},"attestation_state":"computed","paper":{"title":"Abelian p-Form (p = 1, 2, 3) Gauge Theories as the Field Theoretic Models for the Hodge Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Shukla, R. Kumar, R. P. Malik, S. Krishna","submitted_at":"2012-03-25T17:04:00Z","abstract_excerpt":"Taking the simple examples of an Abelian 1-form gauge theory in two (1 + 1)-dimensions, a 2-form gauge theory in four (3 + 1)-dimensions and a 3-form gauge theory in six (5 + 1)-dimensions of spacetime, we establish that such gauge theories respect, in addition to the gauge symmetry transformations that are generated by the first-class constraints of the theory, additional continuous symmetry transformations. We christen the latter symmetry transformations as the dual-gauge transformations. We generalize the above gauge and dual-gauge transformations to obtain the proper (anti-)BRST and (anti-"},"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":"1203.5519","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-03-25T17:04:00Z","cross_cats_sorted":[],"title_canon_sha256":"e7f6400d3ff747f4cb06da668c89e51f21ba6efefd0650317b10c3b05025b062","abstract_canon_sha256":"558ba3bf1121b21b53a2f80effbbb02195d4c7325bdac5237e1ed9d2862f5f3c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:41:59.849650Z","signature_b64":"SW5PeNnoL9EcvhzqUSxocUDM+iwDyqNfw4FL+ZgNEv9+KVYJs38/vtLNzVvt+EjYl7HgVyO+7xQ2SIq0AOPjBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"545443d0b97ff42d0a59273b417b493dea412ecb5bd45fd530f590ca8da6bccd","last_reissued_at":"2026-05-18T02:41:59.849267Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:41:59.849267Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Abelian p-Form (p = 1, 2, 3) Gauge Theories as the Field Theoretic Models for the Hodge Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Shukla, R. Kumar, R. P. Malik, S. Krishna","submitted_at":"2012-03-25T17:04:00Z","abstract_excerpt":"Taking the simple examples of an Abelian 1-form gauge theory in two (1 + 1)-dimensions, a 2-form gauge theory in four (3 + 1)-dimensions and a 3-form gauge theory in six (5 + 1)-dimensions of spacetime, we establish that such gauge theories respect, in addition to the gauge symmetry transformations that are generated by the first-class constraints of the theory, additional continuous symmetry transformations. We christen the latter symmetry transformations as the dual-gauge transformations. We generalize the above gauge and dual-gauge transformations to obtain the proper (anti-)BRST and (anti-"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.5519","kind":"arxiv","version":5},"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":"1203.5519","created_at":"2026-05-18T02:41:59.849324+00:00"},{"alias_kind":"arxiv_version","alias_value":"1203.5519v5","created_at":"2026-05-18T02:41:59.849324+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.5519","created_at":"2026-05-18T02:41:59.849324+00:00"},{"alias_kind":"pith_short_12","alias_value":"KRKEHUFZP72C","created_at":"2026-05-18T12:27:11.947152+00:00"},{"alias_kind":"pith_short_16","alias_value":"KRKEHUFZP72C2CSZ","created_at":"2026-05-18T12:27:11.947152+00:00"},{"alias_kind":"pith_short_8","alias_value":"KRKEHUFZ","created_at":"2026-05-18T12:27:11.947152+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/KRKEHUFZP72C2CSZE45UC62JHX","json":"https://pith.science/pith/KRKEHUFZP72C2CSZE45UC62JHX.json","graph_json":"https://pith.science/api/pith-number/KRKEHUFZP72C2CSZE45UC62JHX/graph.json","events_json":"https://pith.science/api/pith-number/KRKEHUFZP72C2CSZE45UC62JHX/events.json","paper":"https://pith.science/paper/KRKEHUFZ"},"agent_actions":{"view_html":"https://pith.science/pith/KRKEHUFZP72C2CSZE45UC62JHX","download_json":"https://pith.science/pith/KRKEHUFZP72C2CSZE45UC62JHX.json","view_paper":"https://pith.science/paper/KRKEHUFZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1203.5519&json=true","fetch_graph":"https://pith.science/api/pith-number/KRKEHUFZP72C2CSZE45UC62JHX/graph.json","fetch_events":"https://pith.science/api/pith-number/KRKEHUFZP72C2CSZE45UC62JHX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KRKEHUFZP72C2CSZE45UC62JHX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KRKEHUFZP72C2CSZE45UC62JHX/action/storage_attestation","attest_author":"https://pith.science/pith/KRKEHUFZP72C2CSZE45UC62JHX/action/author_attestation","sign_citation":"https://pith.science/pith/KRKEHUFZP72C2CSZE45UC62JHX/action/citation_signature","submit_replication":"https://pith.science/pith/KRKEHUFZP72C2CSZE45UC62JHX/action/replication_record"}},"created_at":"2026-05-18T02:41:59.849324+00:00","updated_at":"2026-05-18T02:41:59.849324+00:00"}