{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:YLQMIXX2GZPMLT45RF472LTRPO","short_pith_number":"pith:YLQMIXX2","schema_version":"1.0","canonical_sha256":"c2e0c45efa365ec5cf9d8979fd2e717b83e5e7a7ca3e5ecc1eb38b0a47ecd02d","source":{"kind":"arxiv","id":"1503.06864","version":3},"attestation_state":"computed","paper":{"title":"Higher Spin Fronsdal Equations from the Exact Renormalization Group","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kewang Jin, Onkar Parrikar, Robert G. Leigh","submitted_at":"2015-03-23T22:19:26Z","abstract_excerpt":"We show that truncating the exact renormalization group equations of free $U(N)$ vector models in the single-trace sector to the linearized level reproduces the Fronsdal equations on $AdS_{d+1}$ for all higher spin fields, with the correct boundary conditions. More precisely, we establish canonical equivalence between the linearized RG equations and the familiar local, second order differential equations on $AdS_{d+1}$, namely the higher spin Fronsdal equations. This result is natural because the second-order bulk equations of motion on $AdS$ simply report the value of the quadratic Casimir 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":"1503.06864","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-03-23T22:19:26Z","cross_cats_sorted":[],"title_canon_sha256":"2713bd062b001a0bfbb0493622c67504ad1c410c292b7b152b16071955d4cef5","abstract_canon_sha256":"6b542999cce832d4b8b6602d347b4da293692a2c67277ca242561ad726e558d4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:53:08.718045Z","signature_b64":"BbVuZIT82wNB2zb/x7jHfJrAGDGCZSnYpIvI0o3gB5rr3GAO0IFWyvhvVaavVeAHHosqgD759drjaC36VDQUCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c2e0c45efa365ec5cf9d8979fd2e717b83e5e7a7ca3e5ecc1eb38b0a47ecd02d","last_reissued_at":"2026-05-18T01:53:08.717400Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:53:08.717400Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher Spin Fronsdal Equations from the Exact Renormalization Group","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kewang Jin, Onkar Parrikar, Robert G. Leigh","submitted_at":"2015-03-23T22:19:26Z","abstract_excerpt":"We show that truncating the exact renormalization group equations of free $U(N)$ vector models in the single-trace sector to the linearized level reproduces the Fronsdal equations on $AdS_{d+1}$ for all higher spin fields, with the correct boundary conditions. More precisely, we establish canonical equivalence between the linearized RG equations and the familiar local, second order differential equations on $AdS_{d+1}$, namely the higher spin Fronsdal equations. This result is natural because the second-order bulk equations of motion on $AdS$ simply report the value of the quadratic Casimir of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.06864","kind":"arxiv","version":3},"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":"1503.06864","created_at":"2026-05-18T01:53:08.717499+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.06864v3","created_at":"2026-05-18T01:53:08.717499+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.06864","created_at":"2026-05-18T01:53:08.717499+00:00"},{"alias_kind":"pith_short_12","alias_value":"YLQMIXX2GZPM","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_16","alias_value":"YLQMIXX2GZPMLT45","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_8","alias_value":"YLQMIXX2","created_at":"2026-05-18T12:29:50.041715+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/YLQMIXX2GZPMLT45RF472LTRPO","json":"https://pith.science/pith/YLQMIXX2GZPMLT45RF472LTRPO.json","graph_json":"https://pith.science/api/pith-number/YLQMIXX2GZPMLT45RF472LTRPO/graph.json","events_json":"https://pith.science/api/pith-number/YLQMIXX2GZPMLT45RF472LTRPO/events.json","paper":"https://pith.science/paper/YLQMIXX2"},"agent_actions":{"view_html":"https://pith.science/pith/YLQMIXX2GZPMLT45RF472LTRPO","download_json":"https://pith.science/pith/YLQMIXX2GZPMLT45RF472LTRPO.json","view_paper":"https://pith.science/paper/YLQMIXX2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.06864&json=true","fetch_graph":"https://pith.science/api/pith-number/YLQMIXX2GZPMLT45RF472LTRPO/graph.json","fetch_events":"https://pith.science/api/pith-number/YLQMIXX2GZPMLT45RF472LTRPO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YLQMIXX2GZPMLT45RF472LTRPO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YLQMIXX2GZPMLT45RF472LTRPO/action/storage_attestation","attest_author":"https://pith.science/pith/YLQMIXX2GZPMLT45RF472LTRPO/action/author_attestation","sign_citation":"https://pith.science/pith/YLQMIXX2GZPMLT45RF472LTRPO/action/citation_signature","submit_replication":"https://pith.science/pith/YLQMIXX2GZPMLT45RF472LTRPO/action/replication_record"}},"created_at":"2026-05-18T01:53:08.717499+00:00","updated_at":"2026-05-18T01:53:08.717499+00:00"}