{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:XV565VL4PV77ZBFNJE7UZCLDRU","short_pith_number":"pith:XV565VL4","schema_version":"1.0","canonical_sha256":"bd7beed57c7d7ffc84ad493f4c89638d03391297f6c8a8767d4038c07a59c6e0","source":{"kind":"arxiv","id":"1308.1222","version":4},"attestation_state":"computed","paper":{"title":"Stability, Tunneling and Flux Changing de Sitter Transitions in the Large Volume String Scenario","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"E. Hatefi, F. Quevedo, R. K. Gupta, S. de Alwis","submitted_at":"2013-08-06T09:59:28Z","abstract_excerpt":"We study the non-perturbative stability of the Large Volume Scenario (LVS) of IIB string compactifications, by analysing transitions mediated by the Brown-Teitelboim (BT) brane nucleations and by Coleman De Luccia tunneling (CDL). We find that, as long as the effective field theory description holds, the LVS AdS minima are stable despite being non-supersymmetric. This opens the possibility of having a CFT dual. Metastable de Sitter vacua behave differently depending on the uplifting mechanism. We find explicit expressions for the different decay rates in terms of exponentials of the volume. Am"},"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":"1308.1222","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-08-06T09:59:28Z","cross_cats_sorted":[],"title_canon_sha256":"f442166d8b4e70c8ba523e832553c9e8907cc3039600b95ea37233459c004ab2","abstract_canon_sha256":"40d59c130c953db2ea1ab2b5625401843b368d0a6f350a3aa979e4d88d647039"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:39.182126Z","signature_b64":"DBC5JpcWeCgSTLbqm7+ATWWVnwHp5R2xfTQYwTBNUDksfKOtGklm3+jpQGvfI9X3LPDX+n4RrhDPJdNyhWh5Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bd7beed57c7d7ffc84ad493f4c89638d03391297f6c8a8767d4038c07a59c6e0","last_reissued_at":"2026-05-18T00:44:39.181724Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:39.181724Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Stability, Tunneling and Flux Changing de Sitter Transitions in the Large Volume String Scenario","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"E. Hatefi, F. Quevedo, R. K. Gupta, S. de Alwis","submitted_at":"2013-08-06T09:59:28Z","abstract_excerpt":"We study the non-perturbative stability of the Large Volume Scenario (LVS) of IIB string compactifications, by analysing transitions mediated by the Brown-Teitelboim (BT) brane nucleations and by Coleman De Luccia tunneling (CDL). We find that, as long as the effective field theory description holds, the LVS AdS minima are stable despite being non-supersymmetric. This opens the possibility of having a CFT dual. Metastable de Sitter vacua behave differently depending on the uplifting mechanism. We find explicit expressions for the different decay rates in terms of exponentials of the volume. Am"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.1222","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1308.1222","created_at":"2026-05-18T00:44:39.181786+00:00"},{"alias_kind":"arxiv_version","alias_value":"1308.1222v4","created_at":"2026-05-18T00:44:39.181786+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.1222","created_at":"2026-05-18T00:44:39.181786+00:00"},{"alias_kind":"pith_short_12","alias_value":"XV565VL4PV77","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_16","alias_value":"XV565VL4PV77ZBFN","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_8","alias_value":"XV565VL4","created_at":"2026-05-18T12:28:06.772260+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2410.21372","citing_title":"Morse-Bott inequalities, Topology Change and Cobordisms to Nothing","ref_index":25,"is_internal_anchor":true},{"citing_arxiv_id":"2605.15276","citing_title":"Bordisms between 9d type IIB supergravities and commutator widths of duality groups","ref_index":74,"is_internal_anchor":true},{"citing_arxiv_id":"2605.05357","citing_title":"Small Vacuum Energy and Tunneling in a Modified Bousso-Polchinski Model","ref_index":62,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XV565VL4PV77ZBFNJE7UZCLDRU","json":"https://pith.science/pith/XV565VL4PV77ZBFNJE7UZCLDRU.json","graph_json":"https://pith.science/api/pith-number/XV565VL4PV77ZBFNJE7UZCLDRU/graph.json","events_json":"https://pith.science/api/pith-number/XV565VL4PV77ZBFNJE7UZCLDRU/events.json","paper":"https://pith.science/paper/XV565VL4"},"agent_actions":{"view_html":"https://pith.science/pith/XV565VL4PV77ZBFNJE7UZCLDRU","download_json":"https://pith.science/pith/XV565VL4PV77ZBFNJE7UZCLDRU.json","view_paper":"https://pith.science/paper/XV565VL4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1308.1222&json=true","fetch_graph":"https://pith.science/api/pith-number/XV565VL4PV77ZBFNJE7UZCLDRU/graph.json","fetch_events":"https://pith.science/api/pith-number/XV565VL4PV77ZBFNJE7UZCLDRU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XV565VL4PV77ZBFNJE7UZCLDRU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XV565VL4PV77ZBFNJE7UZCLDRU/action/storage_attestation","attest_author":"https://pith.science/pith/XV565VL4PV77ZBFNJE7UZCLDRU/action/author_attestation","sign_citation":"https://pith.science/pith/XV565VL4PV77ZBFNJE7UZCLDRU/action/citation_signature","submit_replication":"https://pith.science/pith/XV565VL4PV77ZBFNJE7UZCLDRU/action/replication_record"}},"created_at":"2026-05-18T00:44:39.181786+00:00","updated_at":"2026-05-18T00:44:39.181786+00:00"}