{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:53FN6HXJLRZ7NW7AKPHAYE35H2","short_pith_number":"pith:53FN6HXJ","schema_version":"1.0","canonical_sha256":"eecadf1ee95c73f6dbe053ce0c137d3e9f77f24618c995fd41e13157b9f139b5","source":{"kind":"arxiv","id":"hep-th/0201019","version":1},"attestation_state":"computed","paper":{"title":"Notes On Higher Spin Symmetries","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andrei Mikhailov","submitted_at":"2002-01-04T09:03:22Z","abstract_excerpt":"The strong form of the AdS/CFT correspondence implies that the leading $N$ expressions for the connected correlation functions of the gauge invariant operators in the free ${\\cal N}=4$ supersymmetric Yang-Mills theory with the gauge group SU(N) correspond to the boundary S matrix of the classical interacting theory in the Anti de Sitter space. It was conjectured recently that the theory in the bulk should be a local theory of infinitely many higher spin fields. In this paper we study the free higher spin fields ($N=\\infty$) corresponding to the free scalar fields on the boundary. We explicitly"},"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/0201019","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-01-04T09:03:22Z","cross_cats_sorted":[],"title_canon_sha256":"ea12e72189846cb5110caf6325b26cbb4aa8aa6a803cafbddec32f3c735e9ae8","abstract_canon_sha256":"e7ee5f9c95149e43a7851d3a1f0457faa43618d88e254e01aa7b5392118327d1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:31:44.482124Z","signature_b64":"ahDztoM1u/gF+CgpbalfgHg1gEhMQm9FLVjpYWaFX4uR6qBR17SsiMfAQfiMLOCDXqdcAO3IXuW7UpmoLfM8DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eecadf1ee95c73f6dbe053ce0c137d3e9f77f24618c995fd41e13157b9f139b5","last_reissued_at":"2026-07-04T14:31:44.481779Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:31:44.481779Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Notes On Higher Spin Symmetries","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andrei Mikhailov","submitted_at":"2002-01-04T09:03:22Z","abstract_excerpt":"The strong form of the AdS/CFT correspondence implies that the leading $N$ expressions for the connected correlation functions of the gauge invariant operators in the free ${\\cal N}=4$ supersymmetric Yang-Mills theory with the gauge group SU(N) correspond to the boundary S matrix of the classical interacting theory in the Anti de Sitter space. It was conjectured recently that the theory in the bulk should be a local theory of infinitely many higher spin fields. In this paper we study the free higher spin fields ($N=\\infty$) corresponding to the free scalar fields on the boundary. We explicitly"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0201019","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0201019/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/0201019","created_at":"2026-07-04T14:31:44.481835+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0201019v1","created_at":"2026-07-04T14:31:44.481835+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0201019","created_at":"2026-07-04T14:31:44.481835+00:00"},{"alias_kind":"pith_short_12","alias_value":"53FN6HXJLRZ7","created_at":"2026-07-04T14:31:44.481835+00:00"},{"alias_kind":"pith_short_16","alias_value":"53FN6HXJLRZ7NW7A","created_at":"2026-07-04T14:31:44.481835+00:00"},{"alias_kind":"pith_short_8","alias_value":"53FN6HXJ","created_at":"2026-07-04T14:31:44.481835+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2606.03955","citing_title":"Flat from AdS: in any dimension and for any spin","ref_index":33,"is_internal_anchor":true},{"citing_arxiv_id":"2605.30276","citing_title":"Self-dual holography: four-point AdS/CFT correlators in higher-spin gravity","ref_index":50,"is_internal_anchor":true},{"citing_arxiv_id":"2601.04310","citing_title":"QFT as a set of ODEs","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/53FN6HXJLRZ7NW7AKPHAYE35H2","json":"https://pith.science/pith/53FN6HXJLRZ7NW7AKPHAYE35H2.json","graph_json":"https://pith.science/api/pith-number/53FN6HXJLRZ7NW7AKPHAYE35H2/graph.json","events_json":"https://pith.science/api/pith-number/53FN6HXJLRZ7NW7AKPHAYE35H2/events.json","paper":"https://pith.science/paper/53FN6HXJ"},"agent_actions":{"view_html":"https://pith.science/pith/53FN6HXJLRZ7NW7AKPHAYE35H2","download_json":"https://pith.science/pith/53FN6HXJLRZ7NW7AKPHAYE35H2.json","view_paper":"https://pith.science/paper/53FN6HXJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0201019&json=true","fetch_graph":"https://pith.science/api/pith-number/53FN6HXJLRZ7NW7AKPHAYE35H2/graph.json","fetch_events":"https://pith.science/api/pith-number/53FN6HXJLRZ7NW7AKPHAYE35H2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/53FN6HXJLRZ7NW7AKPHAYE35H2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/53FN6HXJLRZ7NW7AKPHAYE35H2/action/storage_attestation","attest_author":"https://pith.science/pith/53FN6HXJLRZ7NW7AKPHAYE35H2/action/author_attestation","sign_citation":"https://pith.science/pith/53FN6HXJLRZ7NW7AKPHAYE35H2/action/citation_signature","submit_replication":"https://pith.science/pith/53FN6HXJLRZ7NW7AKPHAYE35H2/action/replication_record"}},"created_at":"2026-07-04T14:31:44.481835+00:00","updated_at":"2026-07-04T14:31:44.481835+00:00"}