{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:JBKHBK2Z5XZFFVYLF5JLBI2VAJ","short_pith_number":"pith:JBKHBK2Z","schema_version":"1.0","canonical_sha256":"485470ab59edf252d70b2f52b0a35502713d0ea038018464ef172c4fffdb1913","source":{"kind":"arxiv","id":"2102.08365","version":3},"attestation_state":"computed","paper":{"title":"Integrable bootstrap for AdS3/CFT2 correlation functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alessandro Sfondrini, Burkhard Eden, Dennis le Plat","submitted_at":"2021-02-16T18:50:59Z","abstract_excerpt":"We propose an integrable bootstrap framework for the computation of correlation functions for superstrings in $AdS_3\\times S^3\\times T^4$ backgrounds supported by an arbitrary mixture or Ramond-Ramond and Neveu-Schwarz-Neveu-Schwarz fluxes. The framework extends the \"hexagon tessellation\" approach which was originally proposed for $AdS_5\\times S^5$ and for the first time it demonstrates its applicability to other (less supersymmetric) setups. We work out the hexagon form factor for two-particle states, including its dressing factors which follow from those of the spectral problem, and we show "},"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":"2102.08365","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-02-16T18:50:59Z","cross_cats_sorted":[],"title_canon_sha256":"1be6a7ad3c2812aa8dda6556dfac532936f2d14214599260e42a4688c7d27f22","abstract_canon_sha256":"ed66ffd19ad45c90d89d7dc95cc5ed99564676e616c304c9d5dd4df0cae9508e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:10:02.542480Z","signature_b64":"vRMirKXqwoLoEhnWW4knzUxLSjn4/augnAybJjf23lCInXPwrsrm5rHHJvtFk6etMP6UOCDarRdRrzIoly+xAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"485470ab59edf252d70b2f52b0a35502713d0ea038018464ef172c4fffdb1913","last_reissued_at":"2026-07-05T03:10:02.542061Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:10:02.542061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Integrable bootstrap for AdS3/CFT2 correlation functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alessandro Sfondrini, Burkhard Eden, Dennis le Plat","submitted_at":"2021-02-16T18:50:59Z","abstract_excerpt":"We propose an integrable bootstrap framework for the computation of correlation functions for superstrings in $AdS_3\\times S^3\\times T^4$ backgrounds supported by an arbitrary mixture or Ramond-Ramond and Neveu-Schwarz-Neveu-Schwarz fluxes. The framework extends the \"hexagon tessellation\" approach which was originally proposed for $AdS_5\\times S^5$ and for the first time it demonstrates its applicability to other (less supersymmetric) setups. We work out the hexagon form factor for two-particle states, including its dressing factors which follow from those of the spectral problem, and we show "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2102.08365","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2102.08365/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":"2102.08365","created_at":"2026-07-05T03:10:02.542117+00:00"},{"alias_kind":"arxiv_version","alias_value":"2102.08365v3","created_at":"2026-07-05T03:10:02.542117+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2102.08365","created_at":"2026-07-05T03:10:02.542117+00:00"},{"alias_kind":"pith_short_12","alias_value":"JBKHBK2Z5XZF","created_at":"2026-07-05T03:10:02.542117+00:00"},{"alias_kind":"pith_short_16","alias_value":"JBKHBK2Z5XZFFVYL","created_at":"2026-07-05T03:10:02.542117+00:00"},{"alias_kind":"pith_short_8","alias_value":"JBKHBK2Z","created_at":"2026-07-05T03:10:02.542117+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.12191","citing_title":"Dressing Factors and Mirror Thermodynamic Bethe Ansatz for mixed-flux AdS3/CFT2","ref_index":27,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JBKHBK2Z5XZFFVYLF5JLBI2VAJ","json":"https://pith.science/pith/JBKHBK2Z5XZFFVYLF5JLBI2VAJ.json","graph_json":"https://pith.science/api/pith-number/JBKHBK2Z5XZFFVYLF5JLBI2VAJ/graph.json","events_json":"https://pith.science/api/pith-number/JBKHBK2Z5XZFFVYLF5JLBI2VAJ/events.json","paper":"https://pith.science/paper/JBKHBK2Z"},"agent_actions":{"view_html":"https://pith.science/pith/JBKHBK2Z5XZFFVYLF5JLBI2VAJ","download_json":"https://pith.science/pith/JBKHBK2Z5XZFFVYLF5JLBI2VAJ.json","view_paper":"https://pith.science/paper/JBKHBK2Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2102.08365&json=true","fetch_graph":"https://pith.science/api/pith-number/JBKHBK2Z5XZFFVYLF5JLBI2VAJ/graph.json","fetch_events":"https://pith.science/api/pith-number/JBKHBK2Z5XZFFVYLF5JLBI2VAJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JBKHBK2Z5XZFFVYLF5JLBI2VAJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JBKHBK2Z5XZFFVYLF5JLBI2VAJ/action/storage_attestation","attest_author":"https://pith.science/pith/JBKHBK2Z5XZFFVYLF5JLBI2VAJ/action/author_attestation","sign_citation":"https://pith.science/pith/JBKHBK2Z5XZFFVYLF5JLBI2VAJ/action/citation_signature","submit_replication":"https://pith.science/pith/JBKHBK2Z5XZFFVYLF5JLBI2VAJ/action/replication_record"}},"created_at":"2026-07-05T03:10:02.542117+00:00","updated_at":"2026-07-05T03:10:02.542117+00:00"}