{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:KRCLD2JQ2SWXNZ5KU262BF5E4G","short_pith_number":"pith:KRCLD2JQ","schema_version":"1.0","canonical_sha256":"5444b1e930d4ad76e7aaa6bda097a4e1906280773ae78c1f321f942a5e7af8c4","source":{"kind":"arxiv","id":"1411.4662","version":2},"attestation_state":"computed","paper":{"title":"One- and two-loop checks for the AdS(3) x S(3) x T(4) superstring with mixed flux","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Linus Wulff, Per Sundin","submitted_at":"2014-11-17T21:09:15Z","abstract_excerpt":"We compute the one-loop worldsheet S-matrix for the superstring in AdS(3) x S(3) x T(4) supported by a combination of RR and NSNS flux in the massive sector. In the appropriate regularization scheme it agrees with the S-matrix found from symmetry considerations including the proposed dressing phases. As previously observed in other cases the massless modes decouple from the calculation of one-loop massive mode scattering. We also calculate the correction to the dispersion relation at two loops in the Near-Flat-Space limit and find agreement with a proposal for the form of the exact dispersion "},"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":"1411.4662","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-11-17T21:09:15Z","cross_cats_sorted":[],"title_canon_sha256":"24701db95ec5338fc0c9621e643ad6096894a6bfa64d60f91ddab4ca4e7b5316","abstract_canon_sha256":"5bcdd448c6051dbef644748f4517a152927363568ee040e1a44a00c6a316e1fe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:29.712004Z","signature_b64":"Qkwd9IHX03W0AnDPGTLQlI1DqQb8oePy+/txqjBb8yWB3uvsU7EjI7Z+dHreCT4Ndr0lYinxfyOTJbAHjWRCDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5444b1e930d4ad76e7aaa6bda097a4e1906280773ae78c1f321f942a5e7af8c4","last_reissued_at":"2026-05-18T01:41:29.711346Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:29.711346Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"One- and two-loop checks for the AdS(3) x S(3) x T(4) superstring with mixed flux","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Linus Wulff, Per Sundin","submitted_at":"2014-11-17T21:09:15Z","abstract_excerpt":"We compute the one-loop worldsheet S-matrix for the superstring in AdS(3) x S(3) x T(4) supported by a combination of RR and NSNS flux in the massive sector. In the appropriate regularization scheme it agrees with the S-matrix found from symmetry considerations including the proposed dressing phases. As previously observed in other cases the massless modes decouple from the calculation of one-loop massive mode scattering. We also calculate the correction to the dispersion relation at two loops in the Near-Flat-Space limit and find agreement with a proposal for the form of the exact dispersion "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.4662","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":""},"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":"1411.4662","created_at":"2026-05-18T01:41:29.711452+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.4662v2","created_at":"2026-05-18T01:41:29.711452+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.4662","created_at":"2026-05-18T01:41:29.711452+00:00"},{"alias_kind":"pith_short_12","alias_value":"KRCLD2JQ2SWX","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_16","alias_value":"KRCLD2JQ2SWXNZ5K","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_8","alias_value":"KRCLD2JQ","created_at":"2026-05-18T12:28:35.611951+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":32,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KRCLD2JQ2SWXNZ5KU262BF5E4G","json":"https://pith.science/pith/KRCLD2JQ2SWXNZ5KU262BF5E4G.json","graph_json":"https://pith.science/api/pith-number/KRCLD2JQ2SWXNZ5KU262BF5E4G/graph.json","events_json":"https://pith.science/api/pith-number/KRCLD2JQ2SWXNZ5KU262BF5E4G/events.json","paper":"https://pith.science/paper/KRCLD2JQ"},"agent_actions":{"view_html":"https://pith.science/pith/KRCLD2JQ2SWXNZ5KU262BF5E4G","download_json":"https://pith.science/pith/KRCLD2JQ2SWXNZ5KU262BF5E4G.json","view_paper":"https://pith.science/paper/KRCLD2JQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.4662&json=true","fetch_graph":"https://pith.science/api/pith-number/KRCLD2JQ2SWXNZ5KU262BF5E4G/graph.json","fetch_events":"https://pith.science/api/pith-number/KRCLD2JQ2SWXNZ5KU262BF5E4G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KRCLD2JQ2SWXNZ5KU262BF5E4G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KRCLD2JQ2SWXNZ5KU262BF5E4G/action/storage_attestation","attest_author":"https://pith.science/pith/KRCLD2JQ2SWXNZ5KU262BF5E4G/action/author_attestation","sign_citation":"https://pith.science/pith/KRCLD2JQ2SWXNZ5KU262BF5E4G/action/citation_signature","submit_replication":"https://pith.science/pith/KRCLD2JQ2SWXNZ5KU262BF5E4G/action/replication_record"}},"created_at":"2026-05-18T01:41:29.711452+00:00","updated_at":"2026-05-18T01:41:29.711452+00:00"}