{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:M6CREK4AXI2FILCKUVMVZNKGJQ","short_pith_number":"pith:M6CREK4A","schema_version":"1.0","canonical_sha256":"6785122b80ba34542c4aa5595cb5464c1bf24cfc5bea3ed224caf7b512a2bfdd","source":{"kind":"arxiv","id":"2107.04590","version":1},"attestation_state":"computed","paper":{"title":"The Supersymmetry of Higher-Derivative Supergravity in AdS$_4$ Holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Paul Richmond, Pietro Benetti Genolini","submitted_at":"2021-07-09T17:59:35Z","abstract_excerpt":"An action for the higher-derivative corrections to minimal gauged supergravity in four dimensions has been recently proposed. We demonstrate that the supersymmetric solutions of this model are those of the two-derivative action, and investigate some of their properties. In particular, we prove a formula for the renormalised on-shell action in terms of contributions from fixed points of a $U(1)$ action, and confirm that it is invariant under deformations which preserve the boundary almost contact structure."},"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":"2107.04590","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-07-09T17:59:35Z","cross_cats_sorted":[],"title_canon_sha256":"0808d2342fec34653dd8c4636fa65a1cfe45a02351418c21d398927942f58536","abstract_canon_sha256":"00c42529558b78b11c0656445dd96e7c80d5bc27f290bd34038e24625bc937e9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:14:21.830944Z","signature_b64":"QvFJObixhy1pJLOFeutn1VYZeaP/qT/qM1wttPvtB3bFmlm2kvKt6n9hPpFs+ruUq1b9d+DmLedt0jBXYJyGCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6785122b80ba34542c4aa5595cb5464c1bf24cfc5bea3ed224caf7b512a2bfdd","last_reissued_at":"2026-07-05T03:14:21.830509Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:14:21.830509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Supersymmetry of Higher-Derivative Supergravity in AdS$_4$ Holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Paul Richmond, Pietro Benetti Genolini","submitted_at":"2021-07-09T17:59:35Z","abstract_excerpt":"An action for the higher-derivative corrections to minimal gauged supergravity in four dimensions has been recently proposed. We demonstrate that the supersymmetric solutions of this model are those of the two-derivative action, and investigate some of their properties. In particular, we prove a formula for the renormalised on-shell action in terms of contributions from fixed points of a $U(1)$ action, and confirm that it is invariant under deformations which preserve the boundary almost contact structure."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2107.04590","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/2107.04590/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":"2107.04590","created_at":"2026-07-05T03:14:21.830569+00:00"},{"alias_kind":"arxiv_version","alias_value":"2107.04590v1","created_at":"2026-07-05T03:14:21.830569+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2107.04590","created_at":"2026-07-05T03:14:21.830569+00:00"},{"alias_kind":"pith_short_12","alias_value":"M6CREK4AXI2F","created_at":"2026-07-05T03:14:21.830569+00:00"},{"alias_kind":"pith_short_16","alias_value":"M6CREK4AXI2FILCK","created_at":"2026-07-05T03:14:21.830569+00:00"},{"alias_kind":"pith_short_8","alias_value":"M6CREK4A","created_at":"2026-07-05T03:14:21.830569+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.23893","citing_title":"Towards OSV in AdS","ref_index":93,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08656","citing_title":"Equivariant localization for higher derivative supergravity","ref_index":7,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/M6CREK4AXI2FILCKUVMVZNKGJQ","json":"https://pith.science/pith/M6CREK4AXI2FILCKUVMVZNKGJQ.json","graph_json":"https://pith.science/api/pith-number/M6CREK4AXI2FILCKUVMVZNKGJQ/graph.json","events_json":"https://pith.science/api/pith-number/M6CREK4AXI2FILCKUVMVZNKGJQ/events.json","paper":"https://pith.science/paper/M6CREK4A"},"agent_actions":{"view_html":"https://pith.science/pith/M6CREK4AXI2FILCKUVMVZNKGJQ","download_json":"https://pith.science/pith/M6CREK4AXI2FILCKUVMVZNKGJQ.json","view_paper":"https://pith.science/paper/M6CREK4A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2107.04590&json=true","fetch_graph":"https://pith.science/api/pith-number/M6CREK4AXI2FILCKUVMVZNKGJQ/graph.json","fetch_events":"https://pith.science/api/pith-number/M6CREK4AXI2FILCKUVMVZNKGJQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M6CREK4AXI2FILCKUVMVZNKGJQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M6CREK4AXI2FILCKUVMVZNKGJQ/action/storage_attestation","attest_author":"https://pith.science/pith/M6CREK4AXI2FILCKUVMVZNKGJQ/action/author_attestation","sign_citation":"https://pith.science/pith/M6CREK4AXI2FILCKUVMVZNKGJQ/action/citation_signature","submit_replication":"https://pith.science/pith/M6CREK4AXI2FILCKUVMVZNKGJQ/action/replication_record"}},"created_at":"2026-07-05T03:14:21.830569+00:00","updated_at":"2026-07-05T03:14:21.830569+00:00"}