{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:2WJ5WXLOYL74RNI6AAOT5L2UEZ","short_pith_number":"pith:2WJ5WXLO","schema_version":"1.0","canonical_sha256":"d593db5d6ec2ffc8b51e001d3eaf54267484f5d9d94b0f836fbcaa3aca5b24e0","source":{"kind":"arxiv","id":"2507.16256","version":2},"attestation_state":"computed","paper":{"title":"$T\\bar{T}$-deformed correlators from a 2D gravity description","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Shinji Hirano, Vinayak Raj","submitted_at":"2025-07-22T06:11:56Z","abstract_excerpt":"We study correlators in two-dimensional $T\\bar{T}$-deformed conformal field theories by interpreting the $T\\bar{T}$ deformation as a coupling to two-dimensional gravity. To demonstrate the utility of the massive gravity framework as a particular realization of the gravitational interpretation, we show how the $T\\bar{T}$-deformed correlators at finite coupling can be computed by adopting a judicious parametrization of the 2D metric and a preferred choice of zweibeins. To illustrate how this method works in practice, we compute the leading logarithmic contributions to two- and three-point functi"},"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":"2507.16256","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-07-22T06:11:56Z","cross_cats_sorted":[],"title_canon_sha256":"610d605f8532ff4980ab55e527e8b08efe9fce5348910670d7e3b188cf030256","abstract_canon_sha256":"80cf65f5f16df1604fdd584542de86f17451b4a160207d246ced6256e5702f1f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:43:14.268701Z","signature_b64":"SAtDVlxrkyH/9iRGCTN/AcL9Kv7EfZDjnuxcfY6h4M71GP2wTj7d5wTLNfQqsDN9GQssKl5itIlN93kZfc+KBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d593db5d6ec2ffc8b51e001d3eaf54267484f5d9d94b0f836fbcaa3aca5b24e0","last_reissued_at":"2026-07-05T11:43:14.268199Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:43:14.268199Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$T\\bar{T}$-deformed correlators from a 2D gravity description","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Shinji Hirano, Vinayak Raj","submitted_at":"2025-07-22T06:11:56Z","abstract_excerpt":"We study correlators in two-dimensional $T\\bar{T}$-deformed conformal field theories by interpreting the $T\\bar{T}$ deformation as a coupling to two-dimensional gravity. To demonstrate the utility of the massive gravity framework as a particular realization of the gravitational interpretation, we show how the $T\\bar{T}$-deformed correlators at finite coupling can be computed by adopting a judicious parametrization of the 2D metric and a preferred choice of zweibeins. To illustrate how this method works in practice, we compute the leading logarithmic contributions to two- and three-point functi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.16256","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/2507.16256/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":"2507.16256","created_at":"2026-07-05T11:43:14.268259+00:00"},{"alias_kind":"arxiv_version","alias_value":"2507.16256v2","created_at":"2026-07-05T11:43:14.268259+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.16256","created_at":"2026-07-05T11:43:14.268259+00:00"},{"alias_kind":"pith_short_12","alias_value":"2WJ5WXLOYL74","created_at":"2026-07-05T11:43:14.268259+00:00"},{"alias_kind":"pith_short_16","alias_value":"2WJ5WXLOYL74RNI6","created_at":"2026-07-05T11:43:14.268259+00:00"},{"alias_kind":"pith_short_8","alias_value":"2WJ5WXLO","created_at":"2026-07-05T11:43:14.268259+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.12172","citing_title":"$\\boldsymbol{T\\overline{T}}$ correlators from tensionless strings","ref_index":67,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14939","citing_title":"Correlators in $T\\bar{T}$ and Root-$T\\bar{T}$ Deformed CFTs","ref_index":33,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2WJ5WXLOYL74RNI6AAOT5L2UEZ","json":"https://pith.science/pith/2WJ5WXLOYL74RNI6AAOT5L2UEZ.json","graph_json":"https://pith.science/api/pith-number/2WJ5WXLOYL74RNI6AAOT5L2UEZ/graph.json","events_json":"https://pith.science/api/pith-number/2WJ5WXLOYL74RNI6AAOT5L2UEZ/events.json","paper":"https://pith.science/paper/2WJ5WXLO"},"agent_actions":{"view_html":"https://pith.science/pith/2WJ5WXLOYL74RNI6AAOT5L2UEZ","download_json":"https://pith.science/pith/2WJ5WXLOYL74RNI6AAOT5L2UEZ.json","view_paper":"https://pith.science/paper/2WJ5WXLO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2507.16256&json=true","fetch_graph":"https://pith.science/api/pith-number/2WJ5WXLOYL74RNI6AAOT5L2UEZ/graph.json","fetch_events":"https://pith.science/api/pith-number/2WJ5WXLOYL74RNI6AAOT5L2UEZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2WJ5WXLOYL74RNI6AAOT5L2UEZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2WJ5WXLOYL74RNI6AAOT5L2UEZ/action/storage_attestation","attest_author":"https://pith.science/pith/2WJ5WXLOYL74RNI6AAOT5L2UEZ/action/author_attestation","sign_citation":"https://pith.science/pith/2WJ5WXLOYL74RNI6AAOT5L2UEZ/action/citation_signature","submit_replication":"https://pith.science/pith/2WJ5WXLOYL74RNI6AAOT5L2UEZ/action/replication_record"}},"created_at":"2026-07-05T11:43:14.268259+00:00","updated_at":"2026-07-05T11:43:14.268259+00:00"}