{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:LNKMVFHQDES3IKVMVDROUU473R","short_pith_number":"pith:LNKMVFHQ","schema_version":"1.0","canonical_sha256":"5b54ca94f01925b42aaca8e2ea539fdc6b448d0d28665104b5533ff88e3f9b80","source":{"kind":"arxiv","id":"2303.02120","version":2},"attestation_state":"computed","paper":{"title":"The Tensionless Limit of Pure-Ramond-Ramond AdS3/CFT2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alberto Brollo, Alessandro Sfondrini, Dennis le Plat, Ryo Suzuki","submitted_at":"2023-03-03T18:04:58Z","abstract_excerpt":"Despite impressive advances in the AdS3/CFT2 correspondence, the setup involving Ramond-Ramond backgrounds, which is related to the D1-D5 system of branes, remained relatively poorly understood. We use the Mirror TBA equations recently constructed by Frolov and Sfondrini to study the spectrum of pure Ramond-Ramond $AdS_3\\times S^3\\times T^4$ strings. We find that the leading-order contribution to the anomalous dimensions at small tension is due to the gapless worldsheet excitations, i.e. to the $T^4$ bosons and their superpartners, whose interactions are nontrivial."},"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":"2303.02120","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-03-03T18:04:58Z","cross_cats_sorted":[],"title_canon_sha256":"87407d7dc02a8a127fc612aa521d270718d86080825609e000354458d49ca1f1","abstract_canon_sha256":"abc2c909f2735a981ac6dfcb17959d90b8df6b55547ebe51ba08e2c699b414d4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:12:34.023385Z","signature_b64":"Xp52RHl/Zq6SlCDBGrN2Kp5X5k7hC1/QJDmaj2AtyVRJvaNhCrMtTvBKd0Ag0v5TBrT0t5t0U3eBeg8zEZ6yDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5b54ca94f01925b42aaca8e2ea539fdc6b448d0d28665104b5533ff88e3f9b80","last_reissued_at":"2026-07-05T07:12:34.022995Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:12:34.022995Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Tensionless Limit of Pure-Ramond-Ramond AdS3/CFT2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alberto Brollo, Alessandro Sfondrini, Dennis le Plat, Ryo Suzuki","submitted_at":"2023-03-03T18:04:58Z","abstract_excerpt":"Despite impressive advances in the AdS3/CFT2 correspondence, the setup involving Ramond-Ramond backgrounds, which is related to the D1-D5 system of branes, remained relatively poorly understood. We use the Mirror TBA equations recently constructed by Frolov and Sfondrini to study the spectrum of pure Ramond-Ramond $AdS_3\\times S^3\\times T^4$ strings. We find that the leading-order contribution to the anomalous dimensions at small tension is due to the gapless worldsheet excitations, i.e. to the $T^4$ bosons and their superpartners, whose interactions are nontrivial."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.02120","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/2303.02120/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":"2303.02120","created_at":"2026-07-05T07:12:34.023044+00:00"},{"alias_kind":"arxiv_version","alias_value":"2303.02120v2","created_at":"2026-07-05T07:12:34.023044+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.02120","created_at":"2026-07-05T07:12:34.023044+00:00"},{"alias_kind":"pith_short_12","alias_value":"LNKMVFHQDES3","created_at":"2026-07-05T07:12:34.023044+00:00"},{"alias_kind":"pith_short_16","alias_value":"LNKMVFHQDES3IKVM","created_at":"2026-07-05T07:12:34.023044+00:00"},{"alias_kind":"pith_short_8","alias_value":"LNKMVFHQ","created_at":"2026-07-05T07:12:34.023044+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":42,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LNKMVFHQDES3IKVMVDROUU473R","json":"https://pith.science/pith/LNKMVFHQDES3IKVMVDROUU473R.json","graph_json":"https://pith.science/api/pith-number/LNKMVFHQDES3IKVMVDROUU473R/graph.json","events_json":"https://pith.science/api/pith-number/LNKMVFHQDES3IKVMVDROUU473R/events.json","paper":"https://pith.science/paper/LNKMVFHQ"},"agent_actions":{"view_html":"https://pith.science/pith/LNKMVFHQDES3IKVMVDROUU473R","download_json":"https://pith.science/pith/LNKMVFHQDES3IKVMVDROUU473R.json","view_paper":"https://pith.science/paper/LNKMVFHQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2303.02120&json=true","fetch_graph":"https://pith.science/api/pith-number/LNKMVFHQDES3IKVMVDROUU473R/graph.json","fetch_events":"https://pith.science/api/pith-number/LNKMVFHQDES3IKVMVDROUU473R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LNKMVFHQDES3IKVMVDROUU473R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LNKMVFHQDES3IKVMVDROUU473R/action/storage_attestation","attest_author":"https://pith.science/pith/LNKMVFHQDES3IKVMVDROUU473R/action/author_attestation","sign_citation":"https://pith.science/pith/LNKMVFHQDES3IKVMVDROUU473R/action/citation_signature","submit_replication":"https://pith.science/pith/LNKMVFHQDES3IKVMVDROUU473R/action/replication_record"}},"created_at":"2026-07-05T07:12:34.023044+00:00","updated_at":"2026-07-05T07:12:34.023044+00:00"}