{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:EZSTOSWCVYEEDRDODSRYCL2V24","short_pith_number":"pith:EZSTOSWC","schema_version":"1.0","canonical_sha256":"2665374ac2ae0841c46e1ca3812f55d71f1b8f47d29bafebf28e53337a9744b6","source":{"kind":"arxiv","id":"2603.18248","version":3},"attestation_state":"computed","paper":{"title":"Type IIB Supergravity Action and Holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chanyoung Joung, Geum Lee, Junho Hong, Soumya Adhikari","submitted_at":"2026-03-18T20:12:16Z","abstract_excerpt":"In the prototypical AdS$_5$/CFT$_4$ correspondence, the free energy of $\\mathcal{N}=4$ SU$(N)$ super Yang-Mills theory is commonly reproduced from the Euclidean on-shell action of five-dimensional gauged supergravity -- a consistent truncation of Type IIB supergravity -- rather than computed directly in ten dimensions. A longstanding obstacle to the latter is that the conventional Type IIB pseudo-action evaluated on the $AdS_5\\times S^5$ background vanishes identically, apparently precluding a first-principles holographic comparison. A recent proposal by Kurlyand and Tseytlin, based on the Pas"},"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":"2603.18248","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-03-18T20:12:16Z","cross_cats_sorted":[],"title_canon_sha256":"d8d28d9d0cfd2dea4915cbc77d834ddfc6ec5865f871d452d85187e82ab07aa1","abstract_canon_sha256":"89092408f8b2e4d780102f67f7cdccb4d6c0343d62650e8b9a6c911a8ec5460b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-07T00:15:54.257151Z","signature_b64":"+mveNI/Yb1foDPF3ocUibAPNbGFxkqF5V5mZXopQMobMWxYDj+iViKGL3b4FFgcJKIq6yrOJdPsM5kxhy+KXBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2665374ac2ae0841c46e1ca3812f55d71f1b8f47d29bafebf28e53337a9744b6","last_reissued_at":"2026-07-07T00:15:54.256401Z","signature_status":"signed_v1","first_computed_at":"2026-07-07T00:15:54.256401Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Type IIB Supergravity Action and Holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chanyoung Joung, Geum Lee, Junho Hong, Soumya Adhikari","submitted_at":"2026-03-18T20:12:16Z","abstract_excerpt":"In the prototypical AdS$_5$/CFT$_4$ correspondence, the free energy of $\\mathcal{N}=4$ SU$(N)$ super Yang-Mills theory is commonly reproduced from the Euclidean on-shell action of five-dimensional gauged supergravity -- a consistent truncation of Type IIB supergravity -- rather than computed directly in ten dimensions. A longstanding obstacle to the latter is that the conventional Type IIB pseudo-action evaluated on the $AdS_5\\times S^5$ background vanishes identically, apparently precluding a first-principles holographic comparison. A recent proposal by Kurlyand and Tseytlin, based on the Pas"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.18248","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/2603.18248/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":"2603.18248","created_at":"2026-07-07T00:15:54.256500+00:00"},{"alias_kind":"arxiv_version","alias_value":"2603.18248v3","created_at":"2026-07-07T00:15:54.256500+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.18248","created_at":"2026-07-07T00:15:54.256500+00:00"},{"alias_kind":"pith_short_12","alias_value":"EZSTOSWCVYEE","created_at":"2026-07-07T00:15:54.256500+00:00"},{"alias_kind":"pith_short_16","alias_value":"EZSTOSWCVYEEDRDO","created_at":"2026-07-07T00:15:54.256500+00:00"},{"alias_kind":"pith_short_8","alias_value":"EZSTOSWC","created_at":"2026-07-07T00:15:54.256500+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.18013","citing_title":"Generalised Symmetries and Manifest Duality II: Curved Spacetime","ref_index":12,"is_internal_anchor":true},{"citing_arxiv_id":"2606.01167","citing_title":"One-loop divergences for KK theories on $\\mathrm{AdS}\\times S$ spaces; a reanalysis of $\\mathrm{AdS}_4 \\times S^7\\,\\big/$ ABJM precision holography","ref_index":57,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EZSTOSWCVYEEDRDODSRYCL2V24","json":"https://pith.science/pith/EZSTOSWCVYEEDRDODSRYCL2V24.json","graph_json":"https://pith.science/api/pith-number/EZSTOSWCVYEEDRDODSRYCL2V24/graph.json","events_json":"https://pith.science/api/pith-number/EZSTOSWCVYEEDRDODSRYCL2V24/events.json","paper":"https://pith.science/paper/EZSTOSWC"},"agent_actions":{"view_html":"https://pith.science/pith/EZSTOSWCVYEEDRDODSRYCL2V24","download_json":"https://pith.science/pith/EZSTOSWCVYEEDRDODSRYCL2V24.json","view_paper":"https://pith.science/paper/EZSTOSWC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2603.18248&json=true","fetch_graph":"https://pith.science/api/pith-number/EZSTOSWCVYEEDRDODSRYCL2V24/graph.json","fetch_events":"https://pith.science/api/pith-number/EZSTOSWCVYEEDRDODSRYCL2V24/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EZSTOSWCVYEEDRDODSRYCL2V24/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EZSTOSWCVYEEDRDODSRYCL2V24/action/storage_attestation","attest_author":"https://pith.science/pith/EZSTOSWCVYEEDRDODSRYCL2V24/action/author_attestation","sign_citation":"https://pith.science/pith/EZSTOSWCVYEEDRDODSRYCL2V24/action/citation_signature","submit_replication":"https://pith.science/pith/EZSTOSWCVYEEDRDODSRYCL2V24/action/replication_record"}},"created_at":"2026-07-07T00:15:54.256500+00:00","updated_at":"2026-07-07T00:15:54.256500+00:00"}