{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:H2ANNIQHMFFXUTAW4CPYD2J36X","short_pith_number":"pith:H2ANNIQH","schema_version":"1.0","canonical_sha256":"3e80d6a207614b7a4c16e09f81e93bf5fc99a39084b92e58a9bf5e1ca44ff34b","source":{"kind":"arxiv","id":"1312.3542","version":3},"attestation_state":"computed","paper":{"title":"S-matrix for strings on $\\eta$-deformed AdS5 x S5","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gleb Arutyunov, Riccardo Borsato, Sergey Frolov","submitted_at":"2013-12-12T16:41:53Z","abstract_excerpt":"We determine the bosonic part of the superstring sigma model Lagrangian on $\\eta$-deformed AdS5 x S5, and use it to compute the perturbative world-sheet scattering matrix of bosonic particles of the model. We then compare it with the large string tension limit of the q-deformed S-matrix and find exact agreement."},"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":"1312.3542","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-12T16:41:53Z","cross_cats_sorted":[],"title_canon_sha256":"a1e98d6476688669e34d476382f2b438953a60c88349a0fae40cba3f420eabc4","abstract_canon_sha256":"6d0f636607431fb00caecec48c78611a565f220a88cbe8392a0d60f19ea12336"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:42.330336Z","signature_b64":"lbGwtcZ7ID8+xl7TJdNNM/Lc9iEperp0EGetc5b+2+Pcd8N7Yu3sco0imbFz8puQGzAdVfsjqVfdobTzaBYCDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3e80d6a207614b7a4c16e09f81e93bf5fc99a39084b92e58a9bf5e1ca44ff34b","last_reissued_at":"2026-05-18T01:34:42.329741Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:42.329741Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"S-matrix for strings on $\\eta$-deformed AdS5 x S5","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gleb Arutyunov, Riccardo Borsato, Sergey Frolov","submitted_at":"2013-12-12T16:41:53Z","abstract_excerpt":"We determine the bosonic part of the superstring sigma model Lagrangian on $\\eta$-deformed AdS5 x S5, and use it to compute the perturbative world-sheet scattering matrix of bosonic particles of the model. We then compare it with the large string tension limit of the q-deformed S-matrix and find exact agreement."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.3542","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":""},"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":"1312.3542","created_at":"2026-05-18T01:34:42.329839+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.3542v3","created_at":"2026-05-18T01:34:42.329839+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.3542","created_at":"2026-05-18T01:34:42.329839+00:00"},{"alias_kind":"pith_short_12","alias_value":"H2ANNIQHMFFX","created_at":"2026-05-18T12:27:46.883200+00:00"},{"alias_kind":"pith_short_16","alias_value":"H2ANNIQHMFFXUTAW","created_at":"2026-05-18T12:27:46.883200+00:00"},{"alias_kind":"pith_short_8","alias_value":"H2ANNIQH","created_at":"2026-05-18T12:27:46.883200+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/H2ANNIQHMFFXUTAW4CPYD2J36X","json":"https://pith.science/pith/H2ANNIQHMFFXUTAW4CPYD2J36X.json","graph_json":"https://pith.science/api/pith-number/H2ANNIQHMFFXUTAW4CPYD2J36X/graph.json","events_json":"https://pith.science/api/pith-number/H2ANNIQHMFFXUTAW4CPYD2J36X/events.json","paper":"https://pith.science/paper/H2ANNIQH"},"agent_actions":{"view_html":"https://pith.science/pith/H2ANNIQHMFFXUTAW4CPYD2J36X","download_json":"https://pith.science/pith/H2ANNIQHMFFXUTAW4CPYD2J36X.json","view_paper":"https://pith.science/paper/H2ANNIQH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.3542&json=true","fetch_graph":"https://pith.science/api/pith-number/H2ANNIQHMFFXUTAW4CPYD2J36X/graph.json","fetch_events":"https://pith.science/api/pith-number/H2ANNIQHMFFXUTAW4CPYD2J36X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/H2ANNIQHMFFXUTAW4CPYD2J36X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/H2ANNIQHMFFXUTAW4CPYD2J36X/action/storage_attestation","attest_author":"https://pith.science/pith/H2ANNIQHMFFXUTAW4CPYD2J36X/action/author_attestation","sign_citation":"https://pith.science/pith/H2ANNIQHMFFXUTAW4CPYD2J36X/action/citation_signature","submit_replication":"https://pith.science/pith/H2ANNIQHMFFXUTAW4CPYD2J36X/action/replication_record"}},"created_at":"2026-05-18T01:34:42.329839+00:00","updated_at":"2026-05-18T01:34:42.329839+00:00"}