{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:W33NQ6B3LJEAM5FXU75CLH32HM","short_pith_number":"pith:W33NQ6B3","schema_version":"1.0","canonical_sha256":"b6f6d8783b5a480674b7a7fa259f7a3b3a1db93eb8689a42bf7c1d4dba332967","source":{"kind":"arxiv","id":"1106.4501","version":3},"attestation_state":"computed","paper":{"title":"From Fixed Points to the Fifth Dimension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","gr-qc","hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"Raman Sundrum","submitted_at":"2011-06-22T16:53:09Z","abstract_excerpt":"4D Lorentzian conformal field theory (CFT) is mapped into 5D anti-de Sitter spacetime (AdS), from the viewpoint of \"geometrizing\" conformal current algebra. A large-N expansion of the CFT is shown to lead to (infinitely many) weakly coupled AdS particles, in one-to-one correspondence with minimal-color-singlet CFT primary operators. If all but a finite number of \"protected\" primary operators have very large scaling dimensions, it is shown that there exists a low-AdS-curvature effective field theory regime for the corresponding finite set of AdS particles. Effective 5D gauge theory and General "},"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":"1106.4501","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-06-22T16:53:09Z","cross_cats_sorted":["cond-mat.str-el","gr-qc","hep-ph","nucl-th"],"title_canon_sha256":"2792004adc32e74869816de2d6b0b9a82e64cf338a2a61e3b8c5a93f6136a627","abstract_canon_sha256":"f0adf2d9384dbe24c5711e3895cdc83035772f7628c23932444d3f0fbfda3bf2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:02.978723Z","signature_b64":"l+NpAwq1y25vgSD7jIscamtSfSOD9ES1jLznzZCJGgPAt2fdtNVQyMVDHHXcdq6DZKLg0eyW0y5i51kXxpLTCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b6f6d8783b5a480674b7a7fa259f7a3b3a1db93eb8689a42bf7c1d4dba332967","last_reissued_at":"2026-05-18T03:23:02.978108Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:02.978108Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"From Fixed Points to the Fifth Dimension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","gr-qc","hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"Raman Sundrum","submitted_at":"2011-06-22T16:53:09Z","abstract_excerpt":"4D Lorentzian conformal field theory (CFT) is mapped into 5D anti-de Sitter spacetime (AdS), from the viewpoint of \"geometrizing\" conformal current algebra. A large-N expansion of the CFT is shown to lead to (infinitely many) weakly coupled AdS particles, in one-to-one correspondence with minimal-color-singlet CFT primary operators. If all but a finite number of \"protected\" primary operators have very large scaling dimensions, it is shown that there exists a low-AdS-curvature effective field theory regime for the corresponding finite set of AdS particles. Effective 5D gauge theory and General "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.4501","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":"1106.4501","created_at":"2026-05-18T03:23:02.978208+00:00"},{"alias_kind":"arxiv_version","alias_value":"1106.4501v3","created_at":"2026-05-18T03:23:02.978208+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.4501","created_at":"2026-05-18T03:23:02.978208+00:00"},{"alias_kind":"pith_short_12","alias_value":"W33NQ6B3LJEA","created_at":"2026-05-18T12:26:44.992195+00:00"},{"alias_kind":"pith_short_16","alias_value":"W33NQ6B3LJEAM5FX","created_at":"2026-05-18T12:26:44.992195+00:00"},{"alias_kind":"pith_short_8","alias_value":"W33NQ6B3","created_at":"2026-05-18T12:26:44.992195+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/W33NQ6B3LJEAM5FXU75CLH32HM","json":"https://pith.science/pith/W33NQ6B3LJEAM5FXU75CLH32HM.json","graph_json":"https://pith.science/api/pith-number/W33NQ6B3LJEAM5FXU75CLH32HM/graph.json","events_json":"https://pith.science/api/pith-number/W33NQ6B3LJEAM5FXU75CLH32HM/events.json","paper":"https://pith.science/paper/W33NQ6B3"},"agent_actions":{"view_html":"https://pith.science/pith/W33NQ6B3LJEAM5FXU75CLH32HM","download_json":"https://pith.science/pith/W33NQ6B3LJEAM5FXU75CLH32HM.json","view_paper":"https://pith.science/paper/W33NQ6B3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1106.4501&json=true","fetch_graph":"https://pith.science/api/pith-number/W33NQ6B3LJEAM5FXU75CLH32HM/graph.json","fetch_events":"https://pith.science/api/pith-number/W33NQ6B3LJEAM5FXU75CLH32HM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W33NQ6B3LJEAM5FXU75CLH32HM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W33NQ6B3LJEAM5FXU75CLH32HM/action/storage_attestation","attest_author":"https://pith.science/pith/W33NQ6B3LJEAM5FXU75CLH32HM/action/author_attestation","sign_citation":"https://pith.science/pith/W33NQ6B3LJEAM5FXU75CLH32HM/action/citation_signature","submit_replication":"https://pith.science/pith/W33NQ6B3LJEAM5FXU75CLH32HM/action/replication_record"}},"created_at":"2026-05-18T03:23:02.978208+00:00","updated_at":"2026-05-18T03:23:02.978208+00:00"}