{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:FXQZXDR2OBDYTI3LXATVW4LSJQ","short_pith_number":"pith:FXQZXDR2","schema_version":"1.0","canonical_sha256":"2de19b8e3a704789a36bb8275b71724c347baf7817d3c28a2acf43182c5f9e4c","source":{"kind":"arxiv","id":"1811.03050","version":3},"attestation_state":"computed","paper":{"title":"Holographic integration of $T \\bar{T}$ and $J \\bar{T}$ via $O(d,d)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Eoin \\'O Colg\\'ain, Hossein Yavartanoo, M. M. Sheikh-Jabbari, Thiago Araujo, Yuho Sakatani","submitted_at":"2018-11-07T18:05:46Z","abstract_excerpt":"Prompted by the recent developments in integrable single trace $T \\bar{T}$ and $J \\bar{T}$ deformations of 2d CFTs, we analyse such deformations in the context of $AdS_3/CFT_2$ from the dual string worldsheet CFT viewpoint. We observe that the finite form of these deformations can be recast as $O(d,d)$ transformations, which are an integrated form of the corresponding Exactly Marginal Deformations (EMD) in the worldsheet Wess-Zumino-Witten (WZW) model, thereby generalising the Yang-Baxter class that includes TsT. Furthermore, the equivalence between $O(d,d)$ transformations and marginal deform"},"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":"1811.03050","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-11-07T18:05:46Z","cross_cats_sorted":[],"title_canon_sha256":"f20a823767149d5ad49425c816ba879e6c150c046067310a9410f5fdd6b0debf","abstract_canon_sha256":"030c7469f91cac857ca3fb94b2056425a64751af7a0fc7f9315e5a5e0bdc63ac"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:29.694556Z","signature_b64":"cri7eYz71JQYV1Sqw7RQThbW88yuVtJDw9iH88YdmRG2nzF5T07ooYGgAI+qnUNk8qKPkJP8T+hfSCsxzxoBAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2de19b8e3a704789a36bb8275b71724c347baf7817d3c28a2acf43182c5f9e4c","last_reissued_at":"2026-05-17T23:47:29.693880Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:29.693880Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic integration of $T \\bar{T}$ and $J \\bar{T}$ via $O(d,d)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Eoin \\'O Colg\\'ain, Hossein Yavartanoo, M. M. Sheikh-Jabbari, Thiago Araujo, Yuho Sakatani","submitted_at":"2018-11-07T18:05:46Z","abstract_excerpt":"Prompted by the recent developments in integrable single trace $T \\bar{T}$ and $J \\bar{T}$ deformations of 2d CFTs, we analyse such deformations in the context of $AdS_3/CFT_2$ from the dual string worldsheet CFT viewpoint. We observe that the finite form of these deformations can be recast as $O(d,d)$ transformations, which are an integrated form of the corresponding Exactly Marginal Deformations (EMD) in the worldsheet Wess-Zumino-Witten (WZW) model, thereby generalising the Yang-Baxter class that includes TsT. Furthermore, the equivalence between $O(d,d)$ transformations and marginal deform"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.03050","kind":"arxiv","version":3},"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":"1811.03050","created_at":"2026-05-17T23:47:29.693963+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.03050v3","created_at":"2026-05-17T23:47:29.693963+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.03050","created_at":"2026-05-17T23:47:29.693963+00:00"},{"alias_kind":"pith_short_12","alias_value":"FXQZXDR2OBDY","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_16","alias_value":"FXQZXDR2OBDYTI3L","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_8","alias_value":"FXQZXDR2","created_at":"2026-05-18T12:32:25.280505+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2510.24406","citing_title":"Penrose limits and TsT for fibered $I$-branes","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2602.06113","citing_title":"Deforming the Double-Scaled SYK & Reaching the Stretched Horizon From Finite Cutoff Holography","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FXQZXDR2OBDYTI3LXATVW4LSJQ","json":"https://pith.science/pith/FXQZXDR2OBDYTI3LXATVW4LSJQ.json","graph_json":"https://pith.science/api/pith-number/FXQZXDR2OBDYTI3LXATVW4LSJQ/graph.json","events_json":"https://pith.science/api/pith-number/FXQZXDR2OBDYTI3LXATVW4LSJQ/events.json","paper":"https://pith.science/paper/FXQZXDR2"},"agent_actions":{"view_html":"https://pith.science/pith/FXQZXDR2OBDYTI3LXATVW4LSJQ","download_json":"https://pith.science/pith/FXQZXDR2OBDYTI3LXATVW4LSJQ.json","view_paper":"https://pith.science/paper/FXQZXDR2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.03050&json=true","fetch_graph":"https://pith.science/api/pith-number/FXQZXDR2OBDYTI3LXATVW4LSJQ/graph.json","fetch_events":"https://pith.science/api/pith-number/FXQZXDR2OBDYTI3LXATVW4LSJQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FXQZXDR2OBDYTI3LXATVW4LSJQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FXQZXDR2OBDYTI3LXATVW4LSJQ/action/storage_attestation","attest_author":"https://pith.science/pith/FXQZXDR2OBDYTI3LXATVW4LSJQ/action/author_attestation","sign_citation":"https://pith.science/pith/FXQZXDR2OBDYTI3LXATVW4LSJQ/action/citation_signature","submit_replication":"https://pith.science/pith/FXQZXDR2OBDYTI3LXATVW4LSJQ/action/replication_record"}},"created_at":"2026-05-17T23:47:29.693963+00:00","updated_at":"2026-05-17T23:47:29.693963+00:00"}