{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:TLLXJNDSPB2ASJVMJKODX5FNQE","short_pith_number":"pith:TLLXJNDS","schema_version":"1.0","canonical_sha256":"9ad774b47278740926ac4a9c3bf4ad8102891bb9ddff116d985ede357b0a5110","source":{"kind":"arxiv","id":"1803.05173","version":5},"attestation_state":"computed","paper":{"title":"Constrained BRST-BFV and BRST-BV Lagrangians for half-integer HS fields on $R^{1,d-1}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.DS","math.MP","quant-ph"],"primary_cat":"hep-th","authors_text":"Alexander A. Reshetnyak","submitted_at":"2018-03-14T09:26:17Z","abstract_excerpt":"Gauge invariant Lagrangian descriptions of irreducible and reducible half-integer higher-spin mixed-symmetric massless and massive representations of the Poincare group with off-shell algebraic constraints are constructed within a metric-like formulation in a $d$-dimensional flat space-time on the basis of a suggested constrained BRST approach. A Lorentz-invariant resolution of the BRST complex within the constrained BRST formulations produces a gauge-invariant Fang-Fronsdal Lagrangian entirely in terms of the initial triple gamma-traceless spin-tensor field $\\Psi_{(\\mu)_{n}}$ with gamma-trace"},"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":"1803.05173","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-14T09:26:17Z","cross_cats_sorted":["math-ph","math.DS","math.MP","quant-ph"],"title_canon_sha256":"11007ea2d76b4d7b688499e5432339a176d2650d6cc06c721c7b621b91bd9ce1","abstract_canon_sha256":"63afa51276f9061c6ed4d0785dbf2900a61da904b49e23204820880bf85b57e5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:02:27.890276Z","signature_b64":"peAMBdWH2QrE9R5m6Kj9IH7u4Qjrino77M1xY/IIGkBLKA2zP6ejBCA7Mq4ccKHikfqvrtj+9N7Flf1Hu5xVCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ad774b47278740926ac4a9c3bf4ad8102891bb9ddff116d985ede357b0a5110","last_reissued_at":"2026-05-18T00:02:27.889605Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:02:27.889605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constrained BRST-BFV and BRST-BV Lagrangians for half-integer HS fields on $R^{1,d-1}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.DS","math.MP","quant-ph"],"primary_cat":"hep-th","authors_text":"Alexander A. Reshetnyak","submitted_at":"2018-03-14T09:26:17Z","abstract_excerpt":"Gauge invariant Lagrangian descriptions of irreducible and reducible half-integer higher-spin mixed-symmetric massless and massive representations of the Poincare group with off-shell algebraic constraints are constructed within a metric-like formulation in a $d$-dimensional flat space-time on the basis of a suggested constrained BRST approach. A Lorentz-invariant resolution of the BRST complex within the constrained BRST formulations produces a gauge-invariant Fang-Fronsdal Lagrangian entirely in terms of the initial triple gamma-traceless spin-tensor field $\\Psi_{(\\mu)_{n}}$ with gamma-trace"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.05173","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":"1803.05173","created_at":"2026-05-18T00:02:27.889714+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.05173v5","created_at":"2026-05-18T00:02:27.889714+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.05173","created_at":"2026-05-18T00:02:27.889714+00:00"},{"alias_kind":"pith_short_12","alias_value":"TLLXJNDSPB2A","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_16","alias_value":"TLLXJNDSPB2ASJVM","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_8","alias_value":"TLLXJNDS","created_at":"2026-05-18T12:32:53.628368+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/TLLXJNDSPB2ASJVMJKODX5FNQE","json":"https://pith.science/pith/TLLXJNDSPB2ASJVMJKODX5FNQE.json","graph_json":"https://pith.science/api/pith-number/TLLXJNDSPB2ASJVMJKODX5FNQE/graph.json","events_json":"https://pith.science/api/pith-number/TLLXJNDSPB2ASJVMJKODX5FNQE/events.json","paper":"https://pith.science/paper/TLLXJNDS"},"agent_actions":{"view_html":"https://pith.science/pith/TLLXJNDSPB2ASJVMJKODX5FNQE","download_json":"https://pith.science/pith/TLLXJNDSPB2ASJVMJKODX5FNQE.json","view_paper":"https://pith.science/paper/TLLXJNDS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.05173&json=true","fetch_graph":"https://pith.science/api/pith-number/TLLXJNDSPB2ASJVMJKODX5FNQE/graph.json","fetch_events":"https://pith.science/api/pith-number/TLLXJNDSPB2ASJVMJKODX5FNQE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TLLXJNDSPB2ASJVMJKODX5FNQE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TLLXJNDSPB2ASJVMJKODX5FNQE/action/storage_attestation","attest_author":"https://pith.science/pith/TLLXJNDSPB2ASJVMJKODX5FNQE/action/author_attestation","sign_citation":"https://pith.science/pith/TLLXJNDSPB2ASJVMJKODX5FNQE/action/citation_signature","submit_replication":"https://pith.science/pith/TLLXJNDSPB2ASJVMJKODX5FNQE/action/replication_record"}},"created_at":"2026-05-18T00:02:27.889714+00:00","updated_at":"2026-05-18T00:02:27.889714+00:00"}