{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:VLD4PGADRZJS7A6G7GVZQFGYAF","short_pith_number":"pith:VLD4PGAD","schema_version":"1.0","canonical_sha256":"aac7c798038e532f83c6f9ab9814d8017b261967b547aa483c294160b20bc0e8","source":{"kind":"arxiv","id":"2206.04708","version":2},"attestation_state":"computed","paper":{"title":"Effective Theory of Warped Compactifications and the Implications for KKLT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Lisa Randall, Severin L\\\"ust","submitted_at":"2022-06-09T18:00:18Z","abstract_excerpt":"We argue that effective actions for warped compactifications can be subtle, with large deviations in the effective potential from naive expectations owing to constraint equations from the higher-dimensional metric. We demonstrate this deviation in a careful computation of the effective potential for the conifold deformation parameter of the Klebanov-Strassler solution. The uncorrected naive effective potential for the conifold was previously used to argue that the Klebanov-Strassler background would be destabilized by antibranes placed at the conifold infrared tip unless the flux was uncomfort"},"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":"2206.04708","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-06-09T18:00:18Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"2796a51667ae01f68802264cabe4af0f6ee3e343336eb48d73be2cb044e48a20","abstract_canon_sha256":"30a5e20fcfdf13803a88a5c541f37a6263c0cd06086b027315a3add94e3e7275"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:18:39.208774Z","signature_b64":"K83LA8a0Kqleand93pgWbztx6g+4Dr9kuky1Nic1fHdKI9gPF9JHpJi0mWDsnOk8Ma6o48zhAwot1dZpinrvCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aac7c798038e532f83c6f9ab9814d8017b261967b547aa483c294160b20bc0e8","last_reissued_at":"2026-07-05T08:18:39.208230Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:18:39.208230Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective Theory of Warped Compactifications and the Implications for KKLT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Lisa Randall, Severin L\\\"ust","submitted_at":"2022-06-09T18:00:18Z","abstract_excerpt":"We argue that effective actions for warped compactifications can be subtle, with large deviations in the effective potential from naive expectations owing to constraint equations from the higher-dimensional metric. We demonstrate this deviation in a careful computation of the effective potential for the conifold deformation parameter of the Klebanov-Strassler solution. The uncorrected naive effective potential for the conifold was previously used to argue that the Klebanov-Strassler background would be destabilized by antibranes placed at the conifold infrared tip unless the flux was uncomfort"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.04708","kind":"arxiv","version":2},"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/2206.04708/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":"2206.04708","created_at":"2026-07-05T08:18:39.208290+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.04708v2","created_at":"2026-07-05T08:18:39.208290+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.04708","created_at":"2026-07-05T08:18:39.208290+00:00"},{"alias_kind":"pith_short_12","alias_value":"VLD4PGADRZJS","created_at":"2026-07-05T08:18:39.208290+00:00"},{"alias_kind":"pith_short_16","alias_value":"VLD4PGADRZJS7A6G","created_at":"2026-07-05T08:18:39.208290+00:00"},{"alias_kind":"pith_short_8","alias_value":"VLD4PGAD","created_at":"2026-07-05T08:18:39.208290+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2412.08723","citing_title":"Chiral global embedding of Fibre Inflation with $\\overline{\\rm D3}$ uplift","ref_index":107,"is_internal_anchor":false},{"citing_arxiv_id":"2507.02037","citing_title":"An M-theory dS maximum from Casimir energies on Riemann-flat manifolds","ref_index":26,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VLD4PGADRZJS7A6G7GVZQFGYAF","json":"https://pith.science/pith/VLD4PGADRZJS7A6G7GVZQFGYAF.json","graph_json":"https://pith.science/api/pith-number/VLD4PGADRZJS7A6G7GVZQFGYAF/graph.json","events_json":"https://pith.science/api/pith-number/VLD4PGADRZJS7A6G7GVZQFGYAF/events.json","paper":"https://pith.science/paper/VLD4PGAD"},"agent_actions":{"view_html":"https://pith.science/pith/VLD4PGADRZJS7A6G7GVZQFGYAF","download_json":"https://pith.science/pith/VLD4PGADRZJS7A6G7GVZQFGYAF.json","view_paper":"https://pith.science/paper/VLD4PGAD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.04708&json=true","fetch_graph":"https://pith.science/api/pith-number/VLD4PGADRZJS7A6G7GVZQFGYAF/graph.json","fetch_events":"https://pith.science/api/pith-number/VLD4PGADRZJS7A6G7GVZQFGYAF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VLD4PGADRZJS7A6G7GVZQFGYAF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VLD4PGADRZJS7A6G7GVZQFGYAF/action/storage_attestation","attest_author":"https://pith.science/pith/VLD4PGADRZJS7A6G7GVZQFGYAF/action/author_attestation","sign_citation":"https://pith.science/pith/VLD4PGADRZJS7A6G7GVZQFGYAF/action/citation_signature","submit_replication":"https://pith.science/pith/VLD4PGADRZJS7A6G7GVZQFGYAF/action/replication_record"}},"created_at":"2026-07-05T08:18:39.208290+00:00","updated_at":"2026-07-05T08:18:39.208290+00:00"}