{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:R6HYGEUO24FNL64BOUS62L3LOS","short_pith_number":"pith:R6HYGEUO","schema_version":"1.0","canonical_sha256":"8f8f83128ed70ad5fb817525ed2f6b74accc0a13af3641691bdf8c97f306d9c6","source":{"kind":"arxiv","id":"2502.08215","version":2},"attestation_state":"computed","paper":{"title":"Integer dual dimensions in scale-separated AdS$_3$ from massive IIA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Fotis Farakos, George Tringas","submitted_at":"2025-02-12T08:50:13Z","abstract_excerpt":"We study supersymmetric scale-separated AdS$_3$ flux vacua of massive IIA on G2 orbifolds with smeared orientifold planes. We consider two types of $T^7/Z_2^3$ orbifolds which, with appropriate flux choices, yield integer dual dimensions for the operators corresponding to the closed string scalar fields in the dual CFT. As with all other known examples, the dual conformal dimensions are only parametrically close to integer values."},"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":"2502.08215","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-02-12T08:50:13Z","cross_cats_sorted":[],"title_canon_sha256":"e3255eee6656e8efb66c81ee4057def4dce70228da1bfd6281d1d2e8af2997ee","abstract_canon_sha256":"35936b78ddaedb8a2817618b5518c0f2963d6c337e30c37e5b155c885eaed89a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:31:54.111298Z","signature_b64":"YgUc8utuwEfe95+HRcr3Y+rHIQLSnu+UT/8TKp7Q90XXX9qazRtjgK1dR4OcgPsQJTw78mainJp8dyp0axsJAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8f8f83128ed70ad5fb817525ed2f6b74accc0a13af3641691bdf8c97f306d9c6","last_reissued_at":"2026-07-05T10:31:54.110791Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:31:54.110791Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Integer dual dimensions in scale-separated AdS$_3$ from massive IIA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Fotis Farakos, George Tringas","submitted_at":"2025-02-12T08:50:13Z","abstract_excerpt":"We study supersymmetric scale-separated AdS$_3$ flux vacua of massive IIA on G2 orbifolds with smeared orientifold planes. We consider two types of $T^7/Z_2^3$ orbifolds which, with appropriate flux choices, yield integer dual dimensions for the operators corresponding to the closed string scalar fields in the dual CFT. As with all other known examples, the dual conformal dimensions are only parametrically close to integer values."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.08215","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/2502.08215/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":"2502.08215","created_at":"2026-07-05T10:31:54.110847+00:00"},{"alias_kind":"arxiv_version","alias_value":"2502.08215v2","created_at":"2026-07-05T10:31:54.110847+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.08215","created_at":"2026-07-05T10:31:54.110847+00:00"},{"alias_kind":"pith_short_12","alias_value":"R6HYGEUO24FN","created_at":"2026-07-05T10:31:54.110847+00:00"},{"alias_kind":"pith_short_16","alias_value":"R6HYGEUO24FNL64B","created_at":"2026-07-05T10:31:54.110847+00:00"},{"alias_kind":"pith_short_8","alias_value":"R6HYGEUO","created_at":"2026-07-05T10:31:54.110847+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2607.00789","citing_title":"$\\mathcal{N}=1$ spectra, cubic couplings and the rigid fate of DGKT","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2606.30341","citing_title":"A note on the holographic consistency of DGKT-type vacua with $h^{2,1}=0$","ref_index":18,"is_internal_anchor":false},{"citing_arxiv_id":"2512.11031","citing_title":"A Holographic Constraint on Scale Separation","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06800","citing_title":"$G_2$ flux compactifications","ref_index":6,"is_internal_anchor":false},{"citing_arxiv_id":"2605.07464","citing_title":"Broken and restored: a holographic constraint for AdS vacua with orbifolds","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/R6HYGEUO24FNL64BOUS62L3LOS","json":"https://pith.science/pith/R6HYGEUO24FNL64BOUS62L3LOS.json","graph_json":"https://pith.science/api/pith-number/R6HYGEUO24FNL64BOUS62L3LOS/graph.json","events_json":"https://pith.science/api/pith-number/R6HYGEUO24FNL64BOUS62L3LOS/events.json","paper":"https://pith.science/paper/R6HYGEUO"},"agent_actions":{"view_html":"https://pith.science/pith/R6HYGEUO24FNL64BOUS62L3LOS","download_json":"https://pith.science/pith/R6HYGEUO24FNL64BOUS62L3LOS.json","view_paper":"https://pith.science/paper/R6HYGEUO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2502.08215&json=true","fetch_graph":"https://pith.science/api/pith-number/R6HYGEUO24FNL64BOUS62L3LOS/graph.json","fetch_events":"https://pith.science/api/pith-number/R6HYGEUO24FNL64BOUS62L3LOS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R6HYGEUO24FNL64BOUS62L3LOS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R6HYGEUO24FNL64BOUS62L3LOS/action/storage_attestation","attest_author":"https://pith.science/pith/R6HYGEUO24FNL64BOUS62L3LOS/action/author_attestation","sign_citation":"https://pith.science/pith/R6HYGEUO24FNL64BOUS62L3LOS/action/citation_signature","submit_replication":"https://pith.science/pith/R6HYGEUO24FNL64BOUS62L3LOS/action/replication_record"}},"created_at":"2026-07-05T10:31:54.110847+00:00","updated_at":"2026-07-05T10:31:54.110847+00:00"}