{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:6WURBMP2YQAVOB4IKFOXJI2YKR","short_pith_number":"pith:6WURBMP2","schema_version":"1.0","canonical_sha256":"f5a910b1fac401570788515d74a35854503d3616b096f794ed9d84dff4eaaca2","source":{"kind":"arxiv","id":"1402.2278","version":4},"attestation_state":"computed","paper":{"title":"The gravity dual of supersymmetric gauge theories on a squashed $S^1 \\times S^3$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dario Martelli, Davide Cassani","submitted_at":"2014-02-10T21:00:09Z","abstract_excerpt":"We present a new one-parameter family of supersymmetric solutions deforming AdS_5. This is constructed as an asymptotically locally anti de Sitter (AlAdS) solution of five-dimensional minimal gauged supergravity, with topology R x R^4 and a non-trivial graviphoton field, and can be uplifted to ten or eleven dimensional supergravities. An analytic continuation of this solution yields the gravity dual to a class of four-dimensional N=1 supersymmetric gauge theories on a curved manifold with topology S^1 x S^3, comprising an SU(2) x U(1)-symmetric squashed three-sphere, with a non-trivial backgro"},"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":"1402.2278","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-10T21:00:09Z","cross_cats_sorted":[],"title_canon_sha256":"6b3b9733c5958714ec81afc2f655993ddb10bbc70b50671019bac5b07cf175ec","abstract_canon_sha256":"89e4c8d384ade852f735767f50930571866f23b9a9831f0b4d15dd442bdf7421"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:44:45.760916Z","signature_b64":"bS3t7ZGzB83mZJc1dgJCQ62jh1PKak05O4B2jnumhdYTF9BMLEDuU7KNDKf3fm+Y4aD4nGSU9dpVQvtYIXH7AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f5a910b1fac401570788515d74a35854503d3616b096f794ed9d84dff4eaaca2","last_reissued_at":"2026-05-18T01:44:45.760312Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:44:45.760312Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The gravity dual of supersymmetric gauge theories on a squashed $S^1 \\times S^3$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dario Martelli, Davide Cassani","submitted_at":"2014-02-10T21:00:09Z","abstract_excerpt":"We present a new one-parameter family of supersymmetric solutions deforming AdS_5. This is constructed as an asymptotically locally anti de Sitter (AlAdS) solution of five-dimensional minimal gauged supergravity, with topology R x R^4 and a non-trivial graviphoton field, and can be uplifted to ten or eleven dimensional supergravities. An analytic continuation of this solution yields the gravity dual to a class of four-dimensional N=1 supersymmetric gauge theories on a curved manifold with topology S^1 x S^3, comprising an SU(2) x U(1)-symmetric squashed three-sphere, with a non-trivial backgro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.2278","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":"1402.2278","created_at":"2026-05-18T01:44:45.760450+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.2278v4","created_at":"2026-05-18T01:44:45.760450+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.2278","created_at":"2026-05-18T01:44:45.760450+00:00"},{"alias_kind":"pith_short_12","alias_value":"6WURBMP2YQAV","created_at":"2026-05-18T12:28:16.859392+00:00"},{"alias_kind":"pith_short_16","alias_value":"6WURBMP2YQAVOB4I","created_at":"2026-05-18T12:28:16.859392+00:00"},{"alias_kind":"pith_short_8","alias_value":"6WURBMP2","created_at":"2026-05-18T12:28:16.859392+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.08207","citing_title":"Equivariant localization for $D=5$ gauged supergravity","ref_index":40,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6WURBMP2YQAVOB4IKFOXJI2YKR","json":"https://pith.science/pith/6WURBMP2YQAVOB4IKFOXJI2YKR.json","graph_json":"https://pith.science/api/pith-number/6WURBMP2YQAVOB4IKFOXJI2YKR/graph.json","events_json":"https://pith.science/api/pith-number/6WURBMP2YQAVOB4IKFOXJI2YKR/events.json","paper":"https://pith.science/paper/6WURBMP2"},"agent_actions":{"view_html":"https://pith.science/pith/6WURBMP2YQAVOB4IKFOXJI2YKR","download_json":"https://pith.science/pith/6WURBMP2YQAVOB4IKFOXJI2YKR.json","view_paper":"https://pith.science/paper/6WURBMP2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.2278&json=true","fetch_graph":"https://pith.science/api/pith-number/6WURBMP2YQAVOB4IKFOXJI2YKR/graph.json","fetch_events":"https://pith.science/api/pith-number/6WURBMP2YQAVOB4IKFOXJI2YKR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6WURBMP2YQAVOB4IKFOXJI2YKR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6WURBMP2YQAVOB4IKFOXJI2YKR/action/storage_attestation","attest_author":"https://pith.science/pith/6WURBMP2YQAVOB4IKFOXJI2YKR/action/author_attestation","sign_citation":"https://pith.science/pith/6WURBMP2YQAVOB4IKFOXJI2YKR/action/citation_signature","submit_replication":"https://pith.science/pith/6WURBMP2YQAVOB4IKFOXJI2YKR/action/replication_record"}},"created_at":"2026-05-18T01:44:45.760450+00:00","updated_at":"2026-05-18T01:44:45.760450+00:00"}