{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:KAZISYQCPDPTGGWTM2L36EMVTH","short_pith_number":"pith:KAZISYQC","schema_version":"1.0","canonical_sha256":"503289620278df331ad36697bf119599d4520e627e5f9ed16dc72f6d10c7c95d","source":{"kind":"arxiv","id":"2112.06961","version":3},"attestation_state":"computed","paper":{"title":"AdS$_5$ Holography and Higher-Derivative Supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kiril Hristov, Nikolay Bobev, Valentin Reys","submitted_at":"2021-12-13T19:01:22Z","abstract_excerpt":"We study four-derivative corrections to 5d $\\mathcal{N}=2$ minimal gauged supergravity using tools from conformal supergravity. There are two supersymmetric invariants at the four-derivative order and we show explicitly how to write down the action in the Poincar\\'{e} frame in terms of their coefficients. We apply our results in the context of holography where the four-derivative terms in the supergravity action translate into corrections to the conformal anomalies of the dual 4d $\\mathcal{N}=1$ SCFT. We use these results to study corrections to the entropy of the supersymmetric black string s"},"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":"2112.06961","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-12-13T19:01:22Z","cross_cats_sorted":[],"title_canon_sha256":"8270a0242df7543afeb28386fa07d09c3f7930879885ab3540b992289065bb03","abstract_canon_sha256":"12e94d025c7c73336fbd2625454bc787920efc76bec4354b3c2566582a4b6efe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:19:49.993066Z","signature_b64":"q3AFXa3p2bcFIQO/AYgtrcUuUe0OYmQCccbRxef9cfFOuC6Td7Wx+09NBmxglHwWsKKBYWnSeqFpCp0FsJCeCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"503289620278df331ad36697bf119599d4520e627e5f9ed16dc72f6d10c7c95d","last_reissued_at":"2026-07-05T04:19:49.992600Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:19:49.992600Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"AdS$_5$ Holography and Higher-Derivative Supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kiril Hristov, Nikolay Bobev, Valentin Reys","submitted_at":"2021-12-13T19:01:22Z","abstract_excerpt":"We study four-derivative corrections to 5d $\\mathcal{N}=2$ minimal gauged supergravity using tools from conformal supergravity. There are two supersymmetric invariants at the four-derivative order and we show explicitly how to write down the action in the Poincar\\'{e} frame in terms of their coefficients. We apply our results in the context of holography where the four-derivative terms in the supergravity action translate into corrections to the conformal anomalies of the dual 4d $\\mathcal{N}=1$ SCFT. We use these results to study corrections to the entropy of the supersymmetric black string s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2112.06961","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2112.06961/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":"2112.06961","created_at":"2026-07-05T04:19:49.992653+00:00"},{"alias_kind":"arxiv_version","alias_value":"2112.06961v3","created_at":"2026-07-05T04:19:49.992653+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2112.06961","created_at":"2026-07-05T04:19:49.992653+00:00"},{"alias_kind":"pith_short_12","alias_value":"KAZISYQCPDPT","created_at":"2026-07-05T04:19:49.992653+00:00"},{"alias_kind":"pith_short_16","alias_value":"KAZISYQCPDPTGGWT","created_at":"2026-07-05T04:19:49.992653+00:00"},{"alias_kind":"pith_short_8","alias_value":"KAZISYQC","created_at":"2026-07-05T04:19:49.992653+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.21447","citing_title":"$O(d,d)$ symmetric gravity and finite coupling holography","ref_index":8,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21447","citing_title":"$O(d,d)$ symmetric gravity and finite coupling holography","ref_index":8,"is_internal_anchor":false},{"citing_arxiv_id":"2604.09490","citing_title":"The superconformal index and localizing higher derivative supergravity","ref_index":15,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KAZISYQCPDPTGGWTM2L36EMVTH","json":"https://pith.science/pith/KAZISYQCPDPTGGWTM2L36EMVTH.json","graph_json":"https://pith.science/api/pith-number/KAZISYQCPDPTGGWTM2L36EMVTH/graph.json","events_json":"https://pith.science/api/pith-number/KAZISYQCPDPTGGWTM2L36EMVTH/events.json","paper":"https://pith.science/paper/KAZISYQC"},"agent_actions":{"view_html":"https://pith.science/pith/KAZISYQCPDPTGGWTM2L36EMVTH","download_json":"https://pith.science/pith/KAZISYQCPDPTGGWTM2L36EMVTH.json","view_paper":"https://pith.science/paper/KAZISYQC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2112.06961&json=true","fetch_graph":"https://pith.science/api/pith-number/KAZISYQCPDPTGGWTM2L36EMVTH/graph.json","fetch_events":"https://pith.science/api/pith-number/KAZISYQCPDPTGGWTM2L36EMVTH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KAZISYQCPDPTGGWTM2L36EMVTH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KAZISYQCPDPTGGWTM2L36EMVTH/action/storage_attestation","attest_author":"https://pith.science/pith/KAZISYQCPDPTGGWTM2L36EMVTH/action/author_attestation","sign_citation":"https://pith.science/pith/KAZISYQCPDPTGGWTM2L36EMVTH/action/citation_signature","submit_replication":"https://pith.science/pith/KAZISYQCPDPTGGWTM2L36EMVTH/action/replication_record"}},"created_at":"2026-07-05T04:19:49.992653+00:00","updated_at":"2026-07-05T04:19:49.992653+00:00"}