{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:QOFY74WWVCJKGQQV2TWWHZLIKF","short_pith_number":"pith:QOFY74WW","schema_version":"1.0","canonical_sha256":"838b8ff2d6a892a34215d4ed63e5685146d29c92ffd6ad84d5c1a3950e563d7a","source":{"kind":"arxiv","id":"2001.03563","version":1},"attestation_state":"computed","paper":{"title":"Canonical maps and integrability in $T\\bar T$ deformed 2d CFTs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"George Jorjadze, Stefan Theisen","submitted_at":"2020-01-10T17:04:31Z","abstract_excerpt":"We study $T\\bar T$ deformations of 2d CFTs with periodic boundary conditions. We relate these systems to string models on $\\mathbb{R}\\times {S}^1\\times{\\cal M}$, where $\\cal M$ is the target space of a 2d CFT. The string model in the light cone gauge is identified with the corresponding 2d CFT and in the static gauge it reproduces its $T\\bar T$ deformed system. This relates the deformed system and the initial one by a worldsheet coordinate transformation, which becomes a time dependent canonical map in the Hamiltonian treatment. The deformed Hamiltonian defines the string energy and we express"},"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":"2001.03563","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-01-10T17:04:31Z","cross_cats_sorted":[],"title_canon_sha256":"e41b1f63bb2ca6011b68c661645b56dc5d3c1b69521c8099f57ddc39e79c82ac","abstract_canon_sha256":"55976f566700e1862aed304ac2bafed9f076ae4526cfeb64df74e4cd489db1c7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:32:45.068733Z","signature_b64":"7KLZtUyftExph+tspSk3tgb1dTT6QJOauA9B6d48g0HredQxElr8lw0ZBGkiVkdhc6gu4lYiCej9jZh+i6flDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"838b8ff2d6a892a34215d4ed63e5685146d29c92ffd6ad84d5c1a3950e563d7a","last_reissued_at":"2026-07-05T00:32:45.068283Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:32:45.068283Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Canonical maps and integrability in $T\\bar T$ deformed 2d CFTs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"George Jorjadze, Stefan Theisen","submitted_at":"2020-01-10T17:04:31Z","abstract_excerpt":"We study $T\\bar T$ deformations of 2d CFTs with periodic boundary conditions. We relate these systems to string models on $\\mathbb{R}\\times {S}^1\\times{\\cal M}$, where $\\cal M$ is the target space of a 2d CFT. The string model in the light cone gauge is identified with the corresponding 2d CFT and in the static gauge it reproduces its $T\\bar T$ deformed system. This relates the deformed system and the initial one by a worldsheet coordinate transformation, which becomes a time dependent canonical map in the Hamiltonian treatment. The deformed Hamiltonian defines the string energy and we express"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2001.03563","kind":"arxiv","version":1},"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/2001.03563/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":"2001.03563","created_at":"2026-07-05T00:32:45.068336+00:00"},{"alias_kind":"arxiv_version","alias_value":"2001.03563v1","created_at":"2026-07-05T00:32:45.068336+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2001.03563","created_at":"2026-07-05T00:32:45.068336+00:00"},{"alias_kind":"pith_short_12","alias_value":"QOFY74WWVCJK","created_at":"2026-07-05T00:32:45.068336+00:00"},{"alias_kind":"pith_short_16","alias_value":"QOFY74WWVCJKGQQV","created_at":"2026-07-05T00:32:45.068336+00:00"},{"alias_kind":"pith_short_8","alias_value":"QOFY74WW","created_at":"2026-07-05T00:32:45.068336+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.09170","citing_title":"Stress Tensor Deformations in dS/CFT: Mixed Boundary Conditions, Spectrum Flow and Pseudo Entropy","ref_index":64,"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":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QOFY74WWVCJKGQQV2TWWHZLIKF","json":"https://pith.science/pith/QOFY74WWVCJKGQQV2TWWHZLIKF.json","graph_json":"https://pith.science/api/pith-number/QOFY74WWVCJKGQQV2TWWHZLIKF/graph.json","events_json":"https://pith.science/api/pith-number/QOFY74WWVCJKGQQV2TWWHZLIKF/events.json","paper":"https://pith.science/paper/QOFY74WW"},"agent_actions":{"view_html":"https://pith.science/pith/QOFY74WWVCJKGQQV2TWWHZLIKF","download_json":"https://pith.science/pith/QOFY74WWVCJKGQQV2TWWHZLIKF.json","view_paper":"https://pith.science/paper/QOFY74WW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2001.03563&json=true","fetch_graph":"https://pith.science/api/pith-number/QOFY74WWVCJKGQQV2TWWHZLIKF/graph.json","fetch_events":"https://pith.science/api/pith-number/QOFY74WWVCJKGQQV2TWWHZLIKF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QOFY74WWVCJKGQQV2TWWHZLIKF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QOFY74WWVCJKGQQV2TWWHZLIKF/action/storage_attestation","attest_author":"https://pith.science/pith/QOFY74WWVCJKGQQV2TWWHZLIKF/action/author_attestation","sign_citation":"https://pith.science/pith/QOFY74WWVCJKGQQV2TWWHZLIKF/action/citation_signature","submit_replication":"https://pith.science/pith/QOFY74WWVCJKGQQV2TWWHZLIKF/action/replication_record"}},"created_at":"2026-07-05T00:32:45.068336+00:00","updated_at":"2026-07-05T00:32:45.068336+00:00"}