{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:E44KK5KWTNF5D4MM7LEJ6ZJV5L","short_pith_number":"pith:E44KK5KW","schema_version":"1.0","canonical_sha256":"2738a575569b4bd1f18cfac89f6535eafe2fd52a04ed6316b6711f6df013bcbb","source":{"kind":"arxiv","id":"1512.05994","version":3},"attestation_state":"computed","paper":{"title":"On (Un)Broken Higher-Spin Symmetry in Vector Models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"E.D. Skvortsov","submitted_at":"2015-12-18T15:39:15Z","abstract_excerpt":"The simplest consequences of exact and broken higher-spin symmetry are studied. The one-loop anomalous dimensions of higher-spin currents are determined from the multiplet recombination in the spirit of the modern bootstrap programme: the Wilson-Fisher CFT is studied both in the epsilon-expansion and in the large-N. The bulk implications are briefly addressed: part of the higher-spin theory cubic action is reconstructed; one-loop corrections to the AdS masses of higher-spin fields are discussed."},"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":"1512.05994","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-12-18T15:39:15Z","cross_cats_sorted":[],"title_canon_sha256":"735ec45d04e2d9e5724014ca48da5fd82cc5b760f9deb0f617f0881f47d41e33","abstract_canon_sha256":"90c6ea6532c6383b8b49b7d49976dd9acecef09560c5f3336b395f1c892a1436"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:23:37.646982Z","signature_b64":"UnGhHKcTN5p6hSRJOkQt49DN5ffG2imkMA9RTYwZJ7vP5cEpwcrywJ1NTw+UeSv/h6bEqeqGWQwjTDphjtaxCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2738a575569b4bd1f18cfac89f6535eafe2fd52a04ed6316b6711f6df013bcbb","last_reissued_at":"2026-05-18T01:23:37.646260Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:23:37.646260Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On (Un)Broken Higher-Spin Symmetry in Vector Models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"E.D. Skvortsov","submitted_at":"2015-12-18T15:39:15Z","abstract_excerpt":"The simplest consequences of exact and broken higher-spin symmetry are studied. The one-loop anomalous dimensions of higher-spin currents are determined from the multiplet recombination in the spirit of the modern bootstrap programme: the Wilson-Fisher CFT is studied both in the epsilon-expansion and in the large-N. The bulk implications are briefly addressed: part of the higher-spin theory cubic action is reconstructed; one-loop corrections to the AdS masses of higher-spin fields are discussed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.05994","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":"1512.05994","created_at":"2026-05-18T01:23:37.646395+00:00"},{"alias_kind":"arxiv_version","alias_value":"1512.05994v3","created_at":"2026-05-18T01:23:37.646395+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.05994","created_at":"2026-05-18T01:23:37.646395+00:00"},{"alias_kind":"pith_short_12","alias_value":"E44KK5KWTNF5","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_16","alias_value":"E44KK5KWTNF5D4MM","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_8","alias_value":"E44KK5KW","created_at":"2026-05-18T12:29:17.054201+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.16119","citing_title":"Boundary anomalous dimensions from BCFT: $\\phi^{3}$ theories with a boundary and higher-derivative generalizations","ref_index":48,"is_internal_anchor":true},{"citing_arxiv_id":"2601.08909","citing_title":"The CFT Distance Conjecture and Tensionless String Limits in $\\mathcal N=2$ Quiver Gauge Theories","ref_index":113,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/E44KK5KWTNF5D4MM7LEJ6ZJV5L","json":"https://pith.science/pith/E44KK5KWTNF5D4MM7LEJ6ZJV5L.json","graph_json":"https://pith.science/api/pith-number/E44KK5KWTNF5D4MM7LEJ6ZJV5L/graph.json","events_json":"https://pith.science/api/pith-number/E44KK5KWTNF5D4MM7LEJ6ZJV5L/events.json","paper":"https://pith.science/paper/E44KK5KW"},"agent_actions":{"view_html":"https://pith.science/pith/E44KK5KWTNF5D4MM7LEJ6ZJV5L","download_json":"https://pith.science/pith/E44KK5KWTNF5D4MM7LEJ6ZJV5L.json","view_paper":"https://pith.science/paper/E44KK5KW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1512.05994&json=true","fetch_graph":"https://pith.science/api/pith-number/E44KK5KWTNF5D4MM7LEJ6ZJV5L/graph.json","fetch_events":"https://pith.science/api/pith-number/E44KK5KWTNF5D4MM7LEJ6ZJV5L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/E44KK5KWTNF5D4MM7LEJ6ZJV5L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/E44KK5KWTNF5D4MM7LEJ6ZJV5L/action/storage_attestation","attest_author":"https://pith.science/pith/E44KK5KWTNF5D4MM7LEJ6ZJV5L/action/author_attestation","sign_citation":"https://pith.science/pith/E44KK5KWTNF5D4MM7LEJ6ZJV5L/action/citation_signature","submit_replication":"https://pith.science/pith/E44KK5KWTNF5D4MM7LEJ6ZJV5L/action/replication_record"}},"created_at":"2026-05-18T01:23:37.646395+00:00","updated_at":"2026-05-18T01:23:37.646395+00:00"}