{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:GQF7H6F6KPFACCHS6NS5EQI6FN","short_pith_number":"pith:GQF7H6F6","schema_version":"1.0","canonical_sha256":"340bf3f8be53ca0108f2f365d2411e2b5dca22e78eb9a10be9d214fe7ee8dc15","source":{"kind":"arxiv","id":"hep-th/0207212","version":1},"attestation_state":"computed","paper":{"title":"Conformal Higher Spin Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.Y. Segal","submitted_at":"2002-07-23T16:06:48Z","abstract_excerpt":"We construct gauge theory of interacting symmetric traceless tensor fields of all ranks s=0,1,2,3, ... which generalizes Weyl-invariant dilaton gravity to the higher spin case, in any dimension d>2. The action is given by the trace of the projector to the subspace with positive eigenvalues of an arbitrary hermitian differential operator H, the symmetric tensor fields emerge after expansion of the latter in power series in derivatives. After decomposition in perturbative series around a conformally flat point H=\\Box, the quadratic part of the action breaks up as a sum of free gauge theories of "},"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/0207212","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-07-23T16:06:48Z","cross_cats_sorted":[],"title_canon_sha256":"863ddca6de8baeacb43bc1962f8197e31d0ba29964252fee7672138c72ad9f1a","abstract_canon_sha256":"6996ebba4f1c2162ba0daabb5bb85ef607a568f08ed4918214abeca5279ec3dd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:24:54.997528Z","signature_b64":"Mkjy11fDUSmcCADVxd+xEVwlrSfPA+rsFdN709Cg9LVaQfKaSXpzoyyiHQbLbRrSasIsDQ3EK6/ZwZj990msCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"340bf3f8be53ca0108f2f365d2411e2b5dca22e78eb9a10be9d214fe7ee8dc15","last_reissued_at":"2026-07-04T17:24:54.997172Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:24:54.997172Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Conformal Higher Spin Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.Y. Segal","submitted_at":"2002-07-23T16:06:48Z","abstract_excerpt":"We construct gauge theory of interacting symmetric traceless tensor fields of all ranks s=0,1,2,3, ... which generalizes Weyl-invariant dilaton gravity to the higher spin case, in any dimension d>2. The action is given by the trace of the projector to the subspace with positive eigenvalues of an arbitrary hermitian differential operator H, the symmetric tensor fields emerge after expansion of the latter in power series in derivatives. After decomposition in perturbative series around a conformally flat point H=\\Box, the quadratic part of the action breaks up as a sum of free gauge theories of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0207212","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/0207212/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/0207212","created_at":"2026-07-04T17:24:54.997232+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0207212v1","created_at":"2026-07-04T17:24:54.997232+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0207212","created_at":"2026-07-04T17:24:54.997232+00:00"},{"alias_kind":"pith_short_12","alias_value":"GQF7H6F6KPFA","created_at":"2026-07-04T17:24:54.997232+00:00"},{"alias_kind":"pith_short_16","alias_value":"GQF7H6F6KPFACCHS","created_at":"2026-07-04T17:24:54.997232+00:00"},{"alias_kind":"pith_short_8","alias_value":"GQF7H6F6","created_at":"2026-07-04T17:24:54.997232+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2606.25063","citing_title":"Supersymmetry at BLTP: Recent Progress","ref_index":34,"is_internal_anchor":true},{"citing_arxiv_id":"2606.19173","citing_title":"Higher-spin self-dual gravity from holomorphic planes in twistor space","ref_index":27,"is_internal_anchor":true},{"citing_arxiv_id":"2602.19812","citing_title":"dS$^4$ Metamorphosis","ref_index":47,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GQF7H6F6KPFACCHS6NS5EQI6FN","json":"https://pith.science/pith/GQF7H6F6KPFACCHS6NS5EQI6FN.json","graph_json":"https://pith.science/api/pith-number/GQF7H6F6KPFACCHS6NS5EQI6FN/graph.json","events_json":"https://pith.science/api/pith-number/GQF7H6F6KPFACCHS6NS5EQI6FN/events.json","paper":"https://pith.science/paper/GQF7H6F6"},"agent_actions":{"view_html":"https://pith.science/pith/GQF7H6F6KPFACCHS6NS5EQI6FN","download_json":"https://pith.science/pith/GQF7H6F6KPFACCHS6NS5EQI6FN.json","view_paper":"https://pith.science/paper/GQF7H6F6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0207212&json=true","fetch_graph":"https://pith.science/api/pith-number/GQF7H6F6KPFACCHS6NS5EQI6FN/graph.json","fetch_events":"https://pith.science/api/pith-number/GQF7H6F6KPFACCHS6NS5EQI6FN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GQF7H6F6KPFACCHS6NS5EQI6FN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GQF7H6F6KPFACCHS6NS5EQI6FN/action/storage_attestation","attest_author":"https://pith.science/pith/GQF7H6F6KPFACCHS6NS5EQI6FN/action/author_attestation","sign_citation":"https://pith.science/pith/GQF7H6F6KPFACCHS6NS5EQI6FN/action/citation_signature","submit_replication":"https://pith.science/pith/GQF7H6F6KPFACCHS6NS5EQI6FN/action/replication_record"}},"created_at":"2026-07-04T17:24:54.997232+00:00","updated_at":"2026-07-04T17:24:54.997232+00:00"}