{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:JORPGCJZLFJCS3AROOO4R2N4NQ","short_pith_number":"pith:JORPGCJZ","schema_version":"1.0","canonical_sha256":"4ba2f309395952296c11739dc8e9bc6c0ebee466561d4865e28d50d81f3268a0","source":{"kind":"arxiv","id":"1703.10394","version":1},"attestation_state":"computed","paper":{"title":"BRST renormalization of the first order Yang-Mill theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"J C Taylor, J Frenkel","submitted_at":"2017-03-30T10:36:36Z","abstract_excerpt":"We examine the renormalization of the first order formulation of Yang-Mills theory, by using the BRST idenities. These preserve the gauge invariance of the theory and enable a recursive proof of renormalizability to higher orders in perturbation theory. The renormalization involves non-linear mixings as well as re-scalings of the fields and sources, which lead to a renormalized action at all orders."},"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":"1703.10394","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-03-30T10:36:36Z","cross_cats_sorted":[],"title_canon_sha256":"ea61a72339c44b17298fa7b8d3870379a76382f6dfa099bd97a77bd8bfb80f99","abstract_canon_sha256":"f55f65c05447a3fa271917ef1f3ce4677337e9f307644de26d77835d3df475e5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:51.703494Z","signature_b64":"nQ+saeGD1E5ahMf6l3G0/MYFcC2+I2OUNBMHHb7i1KLOTeVv36I57NUQ1siHp8boG+t53mPSOkqagPxZdWYxCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ba2f309395952296c11739dc8e9bc6c0ebee466561d4865e28d50d81f3268a0","last_reissued_at":"2026-05-18T00:26:51.702810Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:51.702810Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"BRST renormalization of the first order Yang-Mill theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"J C Taylor, J Frenkel","submitted_at":"2017-03-30T10:36:36Z","abstract_excerpt":"We examine the renormalization of the first order formulation of Yang-Mills theory, by using the BRST idenities. These preserve the gauge invariance of the theory and enable a recursive proof of renormalizability to higher orders in perturbation theory. The renormalization involves non-linear mixings as well as re-scalings of the fields and sources, which lead to a renormalized action at all orders."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.10394","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":"1703.10394","created_at":"2026-05-18T00:26:51.702920+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.10394v1","created_at":"2026-05-18T00:26:51.702920+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.10394","created_at":"2026-05-18T00:26:51.702920+00:00"},{"alias_kind":"pith_short_12","alias_value":"JORPGCJZLFJC","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_16","alias_value":"JORPGCJZLFJCS3AR","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_8","alias_value":"JORPGCJZ","created_at":"2026-05-18T12:31:24.725408+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/JORPGCJZLFJCS3AROOO4R2N4NQ","json":"https://pith.science/pith/JORPGCJZLFJCS3AROOO4R2N4NQ.json","graph_json":"https://pith.science/api/pith-number/JORPGCJZLFJCS3AROOO4R2N4NQ/graph.json","events_json":"https://pith.science/api/pith-number/JORPGCJZLFJCS3AROOO4R2N4NQ/events.json","paper":"https://pith.science/paper/JORPGCJZ"},"agent_actions":{"view_html":"https://pith.science/pith/JORPGCJZLFJCS3AROOO4R2N4NQ","download_json":"https://pith.science/pith/JORPGCJZLFJCS3AROOO4R2N4NQ.json","view_paper":"https://pith.science/paper/JORPGCJZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.10394&json=true","fetch_graph":"https://pith.science/api/pith-number/JORPGCJZLFJCS3AROOO4R2N4NQ/graph.json","fetch_events":"https://pith.science/api/pith-number/JORPGCJZLFJCS3AROOO4R2N4NQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JORPGCJZLFJCS3AROOO4R2N4NQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JORPGCJZLFJCS3AROOO4R2N4NQ/action/storage_attestation","attest_author":"https://pith.science/pith/JORPGCJZLFJCS3AROOO4R2N4NQ/action/author_attestation","sign_citation":"https://pith.science/pith/JORPGCJZLFJCS3AROOO4R2N4NQ/action/citation_signature","submit_replication":"https://pith.science/pith/JORPGCJZLFJCS3AROOO4R2N4NQ/action/replication_record"}},"created_at":"2026-05-18T00:26:51.702920+00:00","updated_at":"2026-05-18T00:26:51.702920+00:00"}