{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:W6EO5IQY6I2LAJNPODFNBZOEPO","short_pith_number":"pith:W6EO5IQY","schema_version":"1.0","canonical_sha256":"b788eea218f234b025af70cad0e5c47b81bc96eb58f5b1fa2997c4c6bd7ec52d","source":{"kind":"arxiv","id":"hep-th/0701163","version":2},"attestation_state":"computed","paper":{"title":"Current Exchanges and Unconstrained Higher Spins","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Sagnotti (Scuola Normale Superiore, D. Francia (Chalmers U., France), Goteborg, INFN, Italy), J. Mourad (APC, Pisa, Sweden), U. Paris VII","submitted_at":"2007-01-18T06:48:20Z","abstract_excerpt":"The (Fang-)Fronsdal formulation for free fully symmetric (spinor-) tensors rests on (gamma-)trace constraints on gauge fields and parameters. When these are relaxed, glimpses of the underlying geometry emerge: the field equations extend to non-local expressions involving the higher-spin curvatures, and with only a pair of additional fields an equivalent ``minimal'' local formulation is also possible. In this paper we complete the discussion of the ``minimal'' formulation for fully symmetric (spinor-) tensors, constructing one-parameter families of Lagrangians and extending them to (A)dS backgr"},"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/0701163","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-01-18T06:48:20Z","cross_cats_sorted":[],"title_canon_sha256":"06b592971cd2af5c3adaa43f5c7296f0737c1d9304fe5e74dfe4398ff3f70423","abstract_canon_sha256":"7a87f6a9250de75718726165ea267965cf4d7ce70bdcb05832577efffa15fd03"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:11.386307Z","signature_b64":"30X1UFI5XkVFex7c9Yqj4Hq4Fa3JNZxK5d9GCefX/8T5oOCKVMHjsZbfgubYRE+nCMu2ORKFQk9tECwE7t2ECg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b788eea218f234b025af70cad0e5c47b81bc96eb58f5b1fa2997c4c6bd7ec52d","last_reissued_at":"2026-07-04T15:22:11.385933Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:11.385933Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Current Exchanges and Unconstrained Higher Spins","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Sagnotti (Scuola Normale Superiore, D. Francia (Chalmers U., France), Goteborg, INFN, Italy), J. Mourad (APC, Pisa, Sweden), U. Paris VII","submitted_at":"2007-01-18T06:48:20Z","abstract_excerpt":"The (Fang-)Fronsdal formulation for free fully symmetric (spinor-) tensors rests on (gamma-)trace constraints on gauge fields and parameters. When these are relaxed, glimpses of the underlying geometry emerge: the field equations extend to non-local expressions involving the higher-spin curvatures, and with only a pair of additional fields an equivalent ``minimal'' local formulation is also possible. In this paper we complete the discussion of the ``minimal'' formulation for fully symmetric (spinor-) tensors, constructing one-parameter families of Lagrangians and extending them to (A)dS backgr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0701163","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/0701163/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/0701163","created_at":"2026-07-04T15:22:11.385988+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0701163v2","created_at":"2026-07-04T15:22:11.385988+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0701163","created_at":"2026-07-04T15:22:11.385988+00:00"},{"alias_kind":"pith_short_12","alias_value":"W6EO5IQY6I2L","created_at":"2026-07-04T15:22:11.385988+00:00"},{"alias_kind":"pith_short_16","alias_value":"W6EO5IQY6I2LAJNP","created_at":"2026-07-04T15:22:11.385988+00:00"},{"alias_kind":"pith_short_8","alias_value":"W6EO5IQY","created_at":"2026-07-04T15:22:11.385988+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.20165","citing_title":"Boundary Carroll CFTs: SUSY and Superstrings","ref_index":56,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W6EO5IQY6I2LAJNPODFNBZOEPO","json":"https://pith.science/pith/W6EO5IQY6I2LAJNPODFNBZOEPO.json","graph_json":"https://pith.science/api/pith-number/W6EO5IQY6I2LAJNPODFNBZOEPO/graph.json","events_json":"https://pith.science/api/pith-number/W6EO5IQY6I2LAJNPODFNBZOEPO/events.json","paper":"https://pith.science/paper/W6EO5IQY"},"agent_actions":{"view_html":"https://pith.science/pith/W6EO5IQY6I2LAJNPODFNBZOEPO","download_json":"https://pith.science/pith/W6EO5IQY6I2LAJNPODFNBZOEPO.json","view_paper":"https://pith.science/paper/W6EO5IQY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0701163&json=true","fetch_graph":"https://pith.science/api/pith-number/W6EO5IQY6I2LAJNPODFNBZOEPO/graph.json","fetch_events":"https://pith.science/api/pith-number/W6EO5IQY6I2LAJNPODFNBZOEPO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W6EO5IQY6I2LAJNPODFNBZOEPO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W6EO5IQY6I2LAJNPODFNBZOEPO/action/storage_attestation","attest_author":"https://pith.science/pith/W6EO5IQY6I2LAJNPODFNBZOEPO/action/author_attestation","sign_citation":"https://pith.science/pith/W6EO5IQY6I2LAJNPODFNBZOEPO/action/citation_signature","submit_replication":"https://pith.science/pith/W6EO5IQY6I2LAJNPODFNBZOEPO/action/replication_record"}},"created_at":"2026-07-04T15:22:11.385988+00:00","updated_at":"2026-07-04T15:22:11.385988+00:00"}