{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:RRXX5W4YSYCLU3OH2PUXXX4IIF","short_pith_number":"pith:RRXX5W4Y","schema_version":"1.0","canonical_sha256":"8c6f7edb989604ba6dc7d3e97bdf88416c0ccd589bf03c645310deac6b1bb6e3","source":{"kind":"arxiv","id":"1705.10844","version":2},"attestation_state":"computed","paper":{"title":"String Theory of Supertubes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Emil J. Martinec, Stefano Massai","submitted_at":"2017-05-30T19:58:54Z","abstract_excerpt":"String theory on AdS3 backgrounds arises as an IR limit of Little String Theory on NS5-branes. A wide variety of holographic RG flows from the fivebrane theory in the UV to (orbifolds of) AdS3 in the IR is amenable to exact treatment in worldsheet string theory as a class of null-gauged WZW models. The condensate of stringy winding operators which resolves the near-source structure of fivebranes on the Coulomb branch plays a crucial role in AdS3, revealing stringy structure invisible to the supergravity approximation. The D-brane sector contains precursors of the long strings which dominate bl"},"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":"1705.10844","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-30T19:58:54Z","cross_cats_sorted":[],"title_canon_sha256":"b8112fd2abd2e872879f898eb550f774dbba1f2bf9569768abbf50bb89f5fad7","abstract_canon_sha256":"09a2bcce47f03275330ea8651046cbd8198ddf8b7c23bc37d27b122eaee33b3d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:08:20.480237Z","signature_b64":"r++wvDLgIjIOQqF0POcz09QoH89GOPJbdng3WO9GnXX5bUejHGVGMLbLORKn+mF6OGNKf+e1DQLczUgyRzYpDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c6f7edb989604ba6dc7d3e97bdf88416c0ccd589bf03c645310deac6b1bb6e3","last_reissued_at":"2026-07-05T01:08:20.479798Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:08:20.479798Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"String Theory of Supertubes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Emil J. Martinec, Stefano Massai","submitted_at":"2017-05-30T19:58:54Z","abstract_excerpt":"String theory on AdS3 backgrounds arises as an IR limit of Little String Theory on NS5-branes. A wide variety of holographic RG flows from the fivebrane theory in the UV to (orbifolds of) AdS3 in the IR is amenable to exact treatment in worldsheet string theory as a class of null-gauged WZW models. The condensate of stringy winding operators which resolves the near-source structure of fivebranes on the Coulomb branch plays a crucial role in AdS3, revealing stringy structure invisible to the supergravity approximation. The D-brane sector contains precursors of the long strings which dominate bl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.10844","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/1705.10844/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":"1705.10844","created_at":"2026-07-05T01:08:20.479853+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.10844v2","created_at":"2026-07-05T01:08:20.479853+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.10844","created_at":"2026-07-05T01:08:20.479853+00:00"},{"alias_kind":"pith_short_12","alias_value":"RRXX5W4YSYCL","created_at":"2026-07-05T01:08:20.479853+00:00"},{"alias_kind":"pith_short_16","alias_value":"RRXX5W4YSYCLU3OH","created_at":"2026-07-05T01:08:20.479853+00:00"},{"alias_kind":"pith_short_8","alias_value":"RRXX5W4Y","created_at":"2026-07-05T01:08:20.479853+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.12172","citing_title":"$\\boldsymbol{T\\overline{T}}$ correlators from tensionless strings","ref_index":74,"is_internal_anchor":false},{"citing_arxiv_id":"2601.06697","citing_title":"Lecture notes on strings in AdS$_3$ from the worldsheet and the AdS$_3$/CFT$_2$ duality","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2601.09785","citing_title":"Superball of Strings","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25918","citing_title":"de Sitter in String Theory vs. Gibbons & Hawking","ref_index":30,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RRXX5W4YSYCLU3OH2PUXXX4IIF","json":"https://pith.science/pith/RRXX5W4YSYCLU3OH2PUXXX4IIF.json","graph_json":"https://pith.science/api/pith-number/RRXX5W4YSYCLU3OH2PUXXX4IIF/graph.json","events_json":"https://pith.science/api/pith-number/RRXX5W4YSYCLU3OH2PUXXX4IIF/events.json","paper":"https://pith.science/paper/RRXX5W4Y"},"agent_actions":{"view_html":"https://pith.science/pith/RRXX5W4YSYCLU3OH2PUXXX4IIF","download_json":"https://pith.science/pith/RRXX5W4YSYCLU3OH2PUXXX4IIF.json","view_paper":"https://pith.science/paper/RRXX5W4Y","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.10844&json=true","fetch_graph":"https://pith.science/api/pith-number/RRXX5W4YSYCLU3OH2PUXXX4IIF/graph.json","fetch_events":"https://pith.science/api/pith-number/RRXX5W4YSYCLU3OH2PUXXX4IIF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RRXX5W4YSYCLU3OH2PUXXX4IIF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RRXX5W4YSYCLU3OH2PUXXX4IIF/action/storage_attestation","attest_author":"https://pith.science/pith/RRXX5W4YSYCLU3OH2PUXXX4IIF/action/author_attestation","sign_citation":"https://pith.science/pith/RRXX5W4YSYCLU3OH2PUXXX4IIF/action/citation_signature","submit_replication":"https://pith.science/pith/RRXX5W4YSYCLU3OH2PUXXX4IIF/action/replication_record"}},"created_at":"2026-07-05T01:08:20.479853+00:00","updated_at":"2026-07-05T01:08:20.479853+00:00"}