{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:YI2RYAPZ5ZWMWSGNHTSAR7YYA5","short_pith_number":"pith:YI2RYAPZ","schema_version":"1.0","canonical_sha256":"c2351c01f9ee6ccb48cd3ce408ff18077c3cc0f825b444ddb4e4db4b98416323","source":{"kind":"arxiv","id":"1411.6020","version":1},"attestation_state":"computed","paper":{"title":"Correlation Functions in $\\omega$-Deformed N=6 Supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Borghese, C.N. Pope, E. Sezgin, Y. Pang","submitted_at":"2014-11-21T21:05:30Z","abstract_excerpt":"Gauged N=8 supergravity in four dimensions is now known to admit a deformation characterized by a real parameter $\\omega$ lying in the interval $0\\le\\omega\\le \\pi/8$. We analyse the fluctuations about its anti-de Sitter vacuum, and show that the full N=8 supersymmetry can be maintained by the boundary conditions only for $\\omega=0$. For non-vanishing $\\omega$, and requiring that there be no propagating spin s>1 fields on the boundary, we show that N=3 is the maximum degree of supersymmetry that can be preserved by the boundary conditions. We then construct in detail the consistent truncation o"},"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":"1411.6020","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-11-21T21:05:30Z","cross_cats_sorted":[],"title_canon_sha256":"f938c2a6e48435fbdf329365e67b7348cf2fd70b79b9c3adf71493a037e0ff97","abstract_canon_sha256":"e073b2efb5d308f108f24ea353aa7da78a904a401158f1117bdccce18ef453a7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:26:46.759574Z","signature_b64":"c0X+z/7QgX9jcS5tcQNkcyzhxxPKSoQdotcfXZ1/hFhsvDrxw0QvrmJNhvEqMb8zY2S45+WBuB6MxCs9/arcBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c2351c01f9ee6ccb48cd3ce408ff18077c3cc0f825b444ddb4e4db4b98416323","last_reissued_at":"2026-05-18T02:26:46.759146Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:26:46.759146Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Correlation Functions in $\\omega$-Deformed N=6 Supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Borghese, C.N. Pope, E. Sezgin, Y. Pang","submitted_at":"2014-11-21T21:05:30Z","abstract_excerpt":"Gauged N=8 supergravity in four dimensions is now known to admit a deformation characterized by a real parameter $\\omega$ lying in the interval $0\\le\\omega\\le \\pi/8$. We analyse the fluctuations about its anti-de Sitter vacuum, and show that the full N=8 supersymmetry can be maintained by the boundary conditions only for $\\omega=0$. For non-vanishing $\\omega$, and requiring that there be no propagating spin s>1 fields on the boundary, we show that N=3 is the maximum degree of supersymmetry that can be preserved by the boundary conditions. We then construct in detail the consistent truncation o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.6020","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":""},"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":"1411.6020","created_at":"2026-05-18T02:26:46.759210+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.6020v1","created_at":"2026-05-18T02:26:46.759210+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.6020","created_at":"2026-05-18T02:26:46.759210+00:00"},{"alias_kind":"pith_short_12","alias_value":"YI2RYAPZ5ZWM","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_16","alias_value":"YI2RYAPZ5ZWMWSGN","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_8","alias_value":"YI2RYAPZ","created_at":"2026-05-18T12:28:57.508820+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/YI2RYAPZ5ZWMWSGNHTSAR7YYA5","json":"https://pith.science/pith/YI2RYAPZ5ZWMWSGNHTSAR7YYA5.json","graph_json":"https://pith.science/api/pith-number/YI2RYAPZ5ZWMWSGNHTSAR7YYA5/graph.json","events_json":"https://pith.science/api/pith-number/YI2RYAPZ5ZWMWSGNHTSAR7YYA5/events.json","paper":"https://pith.science/paper/YI2RYAPZ"},"agent_actions":{"view_html":"https://pith.science/pith/YI2RYAPZ5ZWMWSGNHTSAR7YYA5","download_json":"https://pith.science/pith/YI2RYAPZ5ZWMWSGNHTSAR7YYA5.json","view_paper":"https://pith.science/paper/YI2RYAPZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.6020&json=true","fetch_graph":"https://pith.science/api/pith-number/YI2RYAPZ5ZWMWSGNHTSAR7YYA5/graph.json","fetch_events":"https://pith.science/api/pith-number/YI2RYAPZ5ZWMWSGNHTSAR7YYA5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YI2RYAPZ5ZWMWSGNHTSAR7YYA5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YI2RYAPZ5ZWMWSGNHTSAR7YYA5/action/storage_attestation","attest_author":"https://pith.science/pith/YI2RYAPZ5ZWMWSGNHTSAR7YYA5/action/author_attestation","sign_citation":"https://pith.science/pith/YI2RYAPZ5ZWMWSGNHTSAR7YYA5/action/citation_signature","submit_replication":"https://pith.science/pith/YI2RYAPZ5ZWMWSGNHTSAR7YYA5/action/replication_record"}},"created_at":"2026-05-18T02:26:46.759210+00:00","updated_at":"2026-05-18T02:26:46.759210+00:00"}