{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:XQQ5AFVL477QNYQY56D546VMD7","short_pith_number":"pith:XQQ5AFVL","schema_version":"1.0","canonical_sha256":"bc21d016abe7ff06e218ef87de7aac1fefc75eda68b9e184d3318175252b5c5a","source":{"kind":"arxiv","id":"1506.04659","version":2},"attestation_state":"computed","paper":{"title":"Conformal Bootstrap With Slightly Broken Higher Spin Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"hep-th","authors_text":"Alexander Zhiboedov, Luis F. Alday","submitted_at":"2015-06-15T16:35:34Z","abstract_excerpt":"We consider conformal field theories with slightly broken higher spin symmetry in arbitrary spacetime dimensions. We analyze the crossing equation in the double light-cone limit and solve for the anomalous dimensions of higher spin currents $\\gamma_s$ with large spin $s$. The result depends on the symmetries and the spectrum of the unperturbed conformal field theory. We reproduce all known results and make further predictions. In particular we make a prediction for the anomalous dimensions of higher spin currents in the 3d Ising model."},"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":"1506.04659","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-06-15T16:35:34Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"a07f4dd2a9a2ae42d0546e7979d805da05fa8507bd309b0f8f444b83c8c2b958","abstract_canon_sha256":"7885a4f6b5d80d44169ef5ef9d4ab9ef72a7649dd4f1c68ea796d5f59abc02da"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:10:54.244697Z","signature_b64":"8IBdBsuM5kjYIkY2EIGDphmGYFPr7yM7RkEl4WoVyYLJpvvw/2+P0i48aJLHP6sW26hS1pCquEftLyh/d+/GDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bc21d016abe7ff06e218ef87de7aac1fefc75eda68b9e184d3318175252b5c5a","last_reissued_at":"2026-05-18T01:10:54.244016Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:10:54.244016Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Conformal Bootstrap With Slightly Broken Higher Spin Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"hep-th","authors_text":"Alexander Zhiboedov, Luis F. Alday","submitted_at":"2015-06-15T16:35:34Z","abstract_excerpt":"We consider conformal field theories with slightly broken higher spin symmetry in arbitrary spacetime dimensions. We analyze the crossing equation in the double light-cone limit and solve for the anomalous dimensions of higher spin currents $\\gamma_s$ with large spin $s$. The result depends on the symmetries and the spectrum of the unperturbed conformal field theory. We reproduce all known results and make further predictions. In particular we make a prediction for the anomalous dimensions of higher spin currents in the 3d Ising model."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.04659","kind":"arxiv","version":2},"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":"1506.04659","created_at":"2026-05-18T01:10:54.244116+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.04659v2","created_at":"2026-05-18T01:10:54.244116+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.04659","created_at":"2026-05-18T01:10:54.244116+00:00"},{"alias_kind":"pith_short_12","alias_value":"XQQ5AFVL477Q","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_16","alias_value":"XQQ5AFVL477QNYQY","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_8","alias_value":"XQQ5AFVL","created_at":"2026-05-18T12:29:50.041715+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.06422","citing_title":"The analytic bootstrap at finite temperature","ref_index":33,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XQQ5AFVL477QNYQY56D546VMD7","json":"https://pith.science/pith/XQQ5AFVL477QNYQY56D546VMD7.json","graph_json":"https://pith.science/api/pith-number/XQQ5AFVL477QNYQY56D546VMD7/graph.json","events_json":"https://pith.science/api/pith-number/XQQ5AFVL477QNYQY56D546VMD7/events.json","paper":"https://pith.science/paper/XQQ5AFVL"},"agent_actions":{"view_html":"https://pith.science/pith/XQQ5AFVL477QNYQY56D546VMD7","download_json":"https://pith.science/pith/XQQ5AFVL477QNYQY56D546VMD7.json","view_paper":"https://pith.science/paper/XQQ5AFVL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.04659&json=true","fetch_graph":"https://pith.science/api/pith-number/XQQ5AFVL477QNYQY56D546VMD7/graph.json","fetch_events":"https://pith.science/api/pith-number/XQQ5AFVL477QNYQY56D546VMD7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XQQ5AFVL477QNYQY56D546VMD7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XQQ5AFVL477QNYQY56D546VMD7/action/storage_attestation","attest_author":"https://pith.science/pith/XQQ5AFVL477QNYQY56D546VMD7/action/author_attestation","sign_citation":"https://pith.science/pith/XQQ5AFVL477QNYQY56D546VMD7/action/citation_signature","submit_replication":"https://pith.science/pith/XQQ5AFVL477QNYQY56D546VMD7/action/replication_record"}},"created_at":"2026-05-18T01:10:54.244116+00:00","updated_at":"2026-05-18T01:10:54.244116+00:00"}