{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:YG4GAU3J5GJM7JX3GF7LQU3C2N","short_pith_number":"pith:YG4GAU3J","schema_version":"1.0","canonical_sha256":"c1b8605369e992cfa6fb317eb85362d342bb7be2135513a7078a08a0a15deb91","source":{"kind":"arxiv","id":"hep-th/0212185","version":2},"attestation_state":"computed","paper":{"title":"On the geometry of higher-spin gauge fields","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Sagnotti (U. Roma \"Tor Vergata\"), D. Francia","submitted_at":"2002-12-16T18:32:55Z","abstract_excerpt":"We review a recent construction of the free field equations for totally symmetric tensors and tensor-spinors that exhibits the corresponding linearized geometry. These equations are not local for all spins >2, involve unconstrained fields and gauge parameters, rest on the curvatures introduced long ago by de Wit and Freedman, and reduce to the local (Fang-)Fronsdal form upon partial gauge fixing. We also describe how the higher-spin geometry is realized in free String Field Theory, and how the gauge fixing to the light cone can be effected. Finally, we review the essential features of local co"},"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/0212185","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-12-16T18:32:55Z","cross_cats_sorted":[],"title_canon_sha256":"3c666b0de45d43f446ab3e140ebc75c4c10ae8f88fe6c779dfedf2750e58e332","abstract_canon_sha256":"1c23cee4574d5329170b4a0193beedfff81cf2f10ae81d5e5aa96b62812521e8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:35:00.665278Z","signature_b64":"2EtVB8N+Z5rb/ozR/ovaTdAu3LJCqXCyUC485GFYIflu++dlNLJ/fNtu0htNwnx8gJLp3heOkbT5mOmwG7bYBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c1b8605369e992cfa6fb317eb85362d342bb7be2135513a7078a08a0a15deb91","last_reissued_at":"2026-07-04T16:35:00.664850Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:35:00.664850Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the geometry of higher-spin gauge fields","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Sagnotti (U. Roma \"Tor Vergata\"), D. Francia","submitted_at":"2002-12-16T18:32:55Z","abstract_excerpt":"We review a recent construction of the free field equations for totally symmetric tensors and tensor-spinors that exhibits the corresponding linearized geometry. These equations are not local for all spins >2, involve unconstrained fields and gauge parameters, rest on the curvatures introduced long ago by de Wit and Freedman, and reduce to the local (Fang-)Fronsdal form upon partial gauge fixing. We also describe how the higher-spin geometry is realized in free String Field Theory, and how the gauge fixing to the light cone can be effected. Finally, we review the essential features of local co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0212185","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0212185/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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/0212185","created_at":"2026-07-04T16:35:00.664913+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0212185v2","created_at":"2026-07-04T16:35:00.664913+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0212185","created_at":"2026-07-04T16:35:00.664913+00:00"},{"alias_kind":"pith_short_12","alias_value":"YG4GAU3J5GJM","created_at":"2026-07-04T16:35:00.664913+00:00"},{"alias_kind":"pith_short_16","alias_value":"YG4GAU3J5GJM7JX3","created_at":"2026-07-04T16:35:00.664913+00:00"},{"alias_kind":"pith_short_8","alias_value":"YG4GAU3J","created_at":"2026-07-04T16:35:00.664913+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2607.02495","citing_title":"BRST-BV approach to fields in Poincare patch of AdS","ref_index":33,"is_internal_anchor":true},{"citing_arxiv_id":"2606.03955","citing_title":"Flat from AdS: in any dimension and for any spin","ref_index":62,"is_internal_anchor":true},{"citing_arxiv_id":"2604.19155","citing_title":"Gauge-invariant off-shell formulations for 3D massive higher-spin supermultiplets","ref_index":40,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YG4GAU3J5GJM7JX3GF7LQU3C2N","json":"https://pith.science/pith/YG4GAU3J5GJM7JX3GF7LQU3C2N.json","graph_json":"https://pith.science/api/pith-number/YG4GAU3J5GJM7JX3GF7LQU3C2N/graph.json","events_json":"https://pith.science/api/pith-number/YG4GAU3J5GJM7JX3GF7LQU3C2N/events.json","paper":"https://pith.science/paper/YG4GAU3J"},"agent_actions":{"view_html":"https://pith.science/pith/YG4GAU3J5GJM7JX3GF7LQU3C2N","download_json":"https://pith.science/pith/YG4GAU3J5GJM7JX3GF7LQU3C2N.json","view_paper":"https://pith.science/paper/YG4GAU3J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0212185&json=true","fetch_graph":"https://pith.science/api/pith-number/YG4GAU3J5GJM7JX3GF7LQU3C2N/graph.json","fetch_events":"https://pith.science/api/pith-number/YG4GAU3J5GJM7JX3GF7LQU3C2N/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YG4GAU3J5GJM7JX3GF7LQU3C2N/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YG4GAU3J5GJM7JX3GF7LQU3C2N/action/storage_attestation","attest_author":"https://pith.science/pith/YG4GAU3J5GJM7JX3GF7LQU3C2N/action/author_attestation","sign_citation":"https://pith.science/pith/YG4GAU3J5GJM7JX3GF7LQU3C2N/action/citation_signature","submit_replication":"https://pith.science/pith/YG4GAU3J5GJM7JX3GF7LQU3C2N/action/replication_record"}},"created_at":"2026-07-04T16:35:00.664913+00:00","updated_at":"2026-07-04T16:35:00.664913+00:00"}