{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:RRQLNFV2IZFTPL4XYVODNY2QSR","short_pith_number":"pith:RRQLNFV2","schema_version":"1.0","canonical_sha256":"8c60b696ba464b37af97c55c36e35094553274359200ec486f08bff2dbe9b736","source":{"kind":"arxiv","id":"1404.7133","version":2},"attestation_state":"computed","paper":{"title":"Flowing from $AdS_5$ to $AdS_3$ with $T^{1,1}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aristomenis Donos, Jerome P. Gauntlett","submitted_at":"2014-04-28T20:00:05Z","abstract_excerpt":"We construct supersymmetric domain wall solutions of type IIB supergravity that interpolate between $AdS_5\\times T^{1,1}$ in the UV and $AdS_3\\times\\mathbb{R}^2\\times S^2\\times S^3$ solutions in the IR. The $\\mathbb{R}^2$ factor can be replaced with a two-torus and then the solution describes a supersymmetric flow across dimensions, similar to wrapped brane solutions. While the domain wall solutions preserve $(0,2)$ supersymmetry, the $AdS_3$ solutions in the IR have an enhanced $(4,2)$ superconformal supersymmetry and are related by two T-dualities to the $AdS_3\\times S^3\\times S^3\\times S^1$"},"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":"1404.7133","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-04-28T20:00:05Z","cross_cats_sorted":[],"title_canon_sha256":"398ce137c8d583af8098a9cad8d7d24f90b95cc093302e6996dd035e1f02bd5c","abstract_canon_sha256":"0a9ef333717108fb300e36342327c061de0b2b044461c1ef9fc3a27836a63e00"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:43:22.438635Z","signature_b64":"v47KIQd7DGjqRHmS1NpUVvl771pUp72+ZomhhzGJJ+MX5tIA+FWZh3nqLs13YSNMHtGNc814578FcwtTZLEiDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c60b696ba464b37af97c55c36e35094553274359200ec486f08bff2dbe9b736","last_reissued_at":"2026-05-18T01:43:22.438006Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:43:22.438006Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Flowing from $AdS_5$ to $AdS_3$ with $T^{1,1}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aristomenis Donos, Jerome P. Gauntlett","submitted_at":"2014-04-28T20:00:05Z","abstract_excerpt":"We construct supersymmetric domain wall solutions of type IIB supergravity that interpolate between $AdS_5\\times T^{1,1}$ in the UV and $AdS_3\\times\\mathbb{R}^2\\times S^2\\times S^3$ solutions in the IR. The $\\mathbb{R}^2$ factor can be replaced with a two-torus and then the solution describes a supersymmetric flow across dimensions, similar to wrapped brane solutions. While the domain wall solutions preserve $(0,2)$ supersymmetry, the $AdS_3$ solutions in the IR have an enhanced $(4,2)$ superconformal supersymmetry and are related by two T-dualities to the $AdS_3\\times S^3\\times S^3\\times S^1$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.7133","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":""},"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":"1404.7133","created_at":"2026-05-18T01:43:22.438093+00:00"},{"alias_kind":"arxiv_version","alias_value":"1404.7133v2","created_at":"2026-05-18T01:43:22.438093+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.7133","created_at":"2026-05-18T01:43:22.438093+00:00"},{"alias_kind":"pith_short_12","alias_value":"RRQLNFV2IZFT","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_16","alias_value":"RRQLNFV2IZFTPL4X","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_8","alias_value":"RRQLNFV2","created_at":"2026-05-18T12:28:46.137349+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.18942","citing_title":"Covariant unification of holographic c-functions","ref_index":131,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RRQLNFV2IZFTPL4XYVODNY2QSR","json":"https://pith.science/pith/RRQLNFV2IZFTPL4XYVODNY2QSR.json","graph_json":"https://pith.science/api/pith-number/RRQLNFV2IZFTPL4XYVODNY2QSR/graph.json","events_json":"https://pith.science/api/pith-number/RRQLNFV2IZFTPL4XYVODNY2QSR/events.json","paper":"https://pith.science/paper/RRQLNFV2"},"agent_actions":{"view_html":"https://pith.science/pith/RRQLNFV2IZFTPL4XYVODNY2QSR","download_json":"https://pith.science/pith/RRQLNFV2IZFTPL4XYVODNY2QSR.json","view_paper":"https://pith.science/paper/RRQLNFV2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1404.7133&json=true","fetch_graph":"https://pith.science/api/pith-number/RRQLNFV2IZFTPL4XYVODNY2QSR/graph.json","fetch_events":"https://pith.science/api/pith-number/RRQLNFV2IZFTPL4XYVODNY2QSR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RRQLNFV2IZFTPL4XYVODNY2QSR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RRQLNFV2IZFTPL4XYVODNY2QSR/action/storage_attestation","attest_author":"https://pith.science/pith/RRQLNFV2IZFTPL4XYVODNY2QSR/action/author_attestation","sign_citation":"https://pith.science/pith/RRQLNFV2IZFTPL4XYVODNY2QSR/action/citation_signature","submit_replication":"https://pith.science/pith/RRQLNFV2IZFTPL4XYVODNY2QSR/action/replication_record"}},"created_at":"2026-05-18T01:43:22.438093+00:00","updated_at":"2026-05-18T01:43:22.438093+00:00"}