{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:W5CXOFOXT7XYHLC2BYBNLRPM4O","short_pith_number":"pith:W5CXOFOX","schema_version":"1.0","canonical_sha256":"b7457715d79fef83ac5a0e02d5c5ece3aa91da0e0485dab879c7d31c24e7f98c","source":{"kind":"arxiv","id":"2311.00742","version":1},"attestation_state":"computed","paper":{"title":"Cubic and higher-order supergravity couplings for AdS vacua using Exceptional Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Bastien Duboeuf, Emanuel Malek, Henning Samtleben","submitted_at":"2023-11-01T18:00:00Z","abstract_excerpt":"We show how to use Exceptional Field Theory to efficiently compute $n$-point couplings of all Kaluza-Klein modes for vacua that can be uplifted from maximal gauged supergravities to 10/11 dimensions via a consistent truncation. Via the AdS/CFT correspondence, these couplings encode the $n$-point functions of holographic conformal fields theories. Our methods show that these $n$-point couplings are controlled by the $n$-point invariant of scalar harmonics of the maximally symmetric point of the truncation, allowing us to show that infinitely-many $n$-point couplings vanish for any vacua of the "},"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":"2311.00742","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-11-01T18:00:00Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"86ad7546d540a86118775bf7c3e67738f1c2b3146a024acfb1bbaf2362dbe9f4","abstract_canon_sha256":"8464ff4f37abfb94b9cb39fa6e28e092f425e78825a997d6b5ab9b040b08d403"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:08:14.768508Z","signature_b64":"iKd54m+xQANwwID1ywSMppXWB3LsYkhxZDP7yNLpBMmAz7akJ81Aj5PAMMGZW7rPVhJ25lovcgF9/0KF1ljvCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b7457715d79fef83ac5a0e02d5c5ece3aa91da0e0485dab879c7d31c24e7f98c","last_reissued_at":"2026-07-05T07:08:14.768062Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:08:14.768062Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Cubic and higher-order supergravity couplings for AdS vacua using Exceptional Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Bastien Duboeuf, Emanuel Malek, Henning Samtleben","submitted_at":"2023-11-01T18:00:00Z","abstract_excerpt":"We show how to use Exceptional Field Theory to efficiently compute $n$-point couplings of all Kaluza-Klein modes for vacua that can be uplifted from maximal gauged supergravities to 10/11 dimensions via a consistent truncation. Via the AdS/CFT correspondence, these couplings encode the $n$-point functions of holographic conformal fields theories. Our methods show that these $n$-point couplings are controlled by the $n$-point invariant of scalar harmonics of the maximally symmetric point of the truncation, allowing us to show that infinitely-many $n$-point couplings vanish for any vacua of the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.00742","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2311.00742/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2311.00742","created_at":"2026-07-05T07:08:14.768120+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.00742v1","created_at":"2026-07-05T07:08:14.768120+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.00742","created_at":"2026-07-05T07:08:14.768120+00:00"},{"alias_kind":"pith_short_12","alias_value":"W5CXOFOXT7XY","created_at":"2026-07-05T07:08:14.768120+00:00"},{"alias_kind":"pith_short_16","alias_value":"W5CXOFOXT7XYHLC2","created_at":"2026-07-05T07:08:14.768120+00:00"},{"alias_kind":"pith_short_8","alias_value":"W5CXOFOX","created_at":"2026-07-05T07:08:14.768120+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2512.03146","citing_title":"Homotopy transfer for massive Kaluza-Klein modes","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W5CXOFOXT7XYHLC2BYBNLRPM4O","json":"https://pith.science/pith/W5CXOFOXT7XYHLC2BYBNLRPM4O.json","graph_json":"https://pith.science/api/pith-number/W5CXOFOXT7XYHLC2BYBNLRPM4O/graph.json","events_json":"https://pith.science/api/pith-number/W5CXOFOXT7XYHLC2BYBNLRPM4O/events.json","paper":"https://pith.science/paper/W5CXOFOX"},"agent_actions":{"view_html":"https://pith.science/pith/W5CXOFOXT7XYHLC2BYBNLRPM4O","download_json":"https://pith.science/pith/W5CXOFOXT7XYHLC2BYBNLRPM4O.json","view_paper":"https://pith.science/paper/W5CXOFOX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.00742&json=true","fetch_graph":"https://pith.science/api/pith-number/W5CXOFOXT7XYHLC2BYBNLRPM4O/graph.json","fetch_events":"https://pith.science/api/pith-number/W5CXOFOXT7XYHLC2BYBNLRPM4O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W5CXOFOXT7XYHLC2BYBNLRPM4O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W5CXOFOXT7XYHLC2BYBNLRPM4O/action/storage_attestation","attest_author":"https://pith.science/pith/W5CXOFOXT7XYHLC2BYBNLRPM4O/action/author_attestation","sign_citation":"https://pith.science/pith/W5CXOFOXT7XYHLC2BYBNLRPM4O/action/citation_signature","submit_replication":"https://pith.science/pith/W5CXOFOXT7XYHLC2BYBNLRPM4O/action/replication_record"}},"created_at":"2026-07-05T07:08:14.768120+00:00","updated_at":"2026-07-05T07:08:14.768120+00:00"}