{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:DUFL6DQYCSR5W3XZDRPFQEHL2J","short_pith_number":"pith:DUFL6DQY","schema_version":"1.0","canonical_sha256":"1d0abf0e1814a3db6ef91c5e5810ebd278e9d297aedab9f16fbde9dad4a32236","source":{"kind":"arxiv","id":"1104.0164","version":1},"attestation_state":"computed","paper":{"title":"The Jackiw-Pi model and its symmetries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"O.M. Del Cima","submitted_at":"2011-04-01T13:19:52Z","abstract_excerpt":"The non-Abelian gauge model proposed by Jackiw and Pi, which generates an even-parity mass term in three space-time dimensions, is revisited in this letter. All the symmetries of the model are collected and established by means of BRS invariance and Slavnov-Taylor identity. The path for the perturbatively quantization of the Jackiw-Pi model, through the algebraic method of renormalization, is presented."},"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":"1104.0164","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-01T13:19:52Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"a9f2793b418868da0605ae3eb275833ccd8c7aa39a702dcaa0907dd8cad019b3","abstract_canon_sha256":"de67e723479e56c99a2f6d3ea72e2901c498a39da964975451e238f6bb319c6c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:14:47.203617Z","signature_b64":"xl0o4XAzJXeO1LRzu92jHRSGUeUqxlB+5hTS0CCZhrt6j8YWQ9hXFSLMr313PifvXxLyj26e0nvZtItDH/QGAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1d0abf0e1814a3db6ef91c5e5810ebd278e9d297aedab9f16fbde9dad4a32236","last_reissued_at":"2026-05-18T04:14:47.203192Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:14:47.203192Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Jackiw-Pi model and its symmetries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"O.M. Del Cima","submitted_at":"2011-04-01T13:19:52Z","abstract_excerpt":"The non-Abelian gauge model proposed by Jackiw and Pi, which generates an even-parity mass term in three space-time dimensions, is revisited in this letter. All the symmetries of the model are collected and established by means of BRS invariance and Slavnov-Taylor identity. The path for the perturbatively quantization of the Jackiw-Pi model, through the algebraic method of renormalization, is presented."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.0164","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":"1104.0164","created_at":"2026-05-18T04:14:47.203241+00:00"},{"alias_kind":"arxiv_version","alias_value":"1104.0164v1","created_at":"2026-05-18T04:14:47.203241+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.0164","created_at":"2026-05-18T04:14:47.203241+00:00"},{"alias_kind":"pith_short_12","alias_value":"DUFL6DQYCSR5","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_16","alias_value":"DUFL6DQYCSR5W3XZ","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_8","alias_value":"DUFL6DQY","created_at":"2026-05-18T12:26:26.731475+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/DUFL6DQYCSR5W3XZDRPFQEHL2J","json":"https://pith.science/pith/DUFL6DQYCSR5W3XZDRPFQEHL2J.json","graph_json":"https://pith.science/api/pith-number/DUFL6DQYCSR5W3XZDRPFQEHL2J/graph.json","events_json":"https://pith.science/api/pith-number/DUFL6DQYCSR5W3XZDRPFQEHL2J/events.json","paper":"https://pith.science/paper/DUFL6DQY"},"agent_actions":{"view_html":"https://pith.science/pith/DUFL6DQYCSR5W3XZDRPFQEHL2J","download_json":"https://pith.science/pith/DUFL6DQYCSR5W3XZDRPFQEHL2J.json","view_paper":"https://pith.science/paper/DUFL6DQY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1104.0164&json=true","fetch_graph":"https://pith.science/api/pith-number/DUFL6DQYCSR5W3XZDRPFQEHL2J/graph.json","fetch_events":"https://pith.science/api/pith-number/DUFL6DQYCSR5W3XZDRPFQEHL2J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DUFL6DQYCSR5W3XZDRPFQEHL2J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DUFL6DQYCSR5W3XZDRPFQEHL2J/action/storage_attestation","attest_author":"https://pith.science/pith/DUFL6DQYCSR5W3XZDRPFQEHL2J/action/author_attestation","sign_citation":"https://pith.science/pith/DUFL6DQYCSR5W3XZDRPFQEHL2J/action/citation_signature","submit_replication":"https://pith.science/pith/DUFL6DQYCSR5W3XZDRPFQEHL2J/action/replication_record"}},"created_at":"2026-05-18T04:14:47.203241+00:00","updated_at":"2026-05-18T04:14:47.203241+00:00"}