{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:NOFDPQXFANKZDDJK6TCTCUS6H6","short_pith_number":"pith:NOFDPQXF","schema_version":"1.0","canonical_sha256":"6b8a37c2e50355918d2af4c531525e3fa18cf31e0cc6b7c473208d25a4c0ed5a","source":{"kind":"arxiv","id":"1306.1930","version":4},"attestation_state":"computed","paper":{"title":"Correlation Functions of the SU(infinity) Principal Chiral Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-lat","nlin.SI"],"primary_cat":"hep-th","authors_text":"Axel Cortes Cubero, Peter Orland","submitted_at":"2013-06-08T15:25:52Z","abstract_excerpt":"We obtain exact matrix elements of physical operators of the (1+1)-dimensional nonlinear sigma model of an SU(N)-valued bare field, in the 't Hooft limit N goes to infinity. Specifically, all the form factors of the Noether current and the stress-energy-momentum tensor are found with an integrable bootstrap method. These form factors are used to find vacuum expectation values of products of these operators."},"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":"1306.1930","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-06-08T15:25:52Z","cross_cats_sorted":["cond-mat.str-el","hep-lat","nlin.SI"],"title_canon_sha256":"0dd5113607bea033cf6678474c39a1e6830f474285cbf7dba3ca02bf9af62966","abstract_canon_sha256":"ca8d1667e9021a160132195f4ba50856344ff6434237c37b45303a82e8d0dd1e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:49:24.644201Z","signature_b64":"4BjKMPWtbK+LnypP+kr8/nYjK52+CFDX9z9IXHNTBQbPYZObSO1Vl7AH3BslVuzZuWiLn5f2JiOL02bgrmfpBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6b8a37c2e50355918d2af4c531525e3fa18cf31e0cc6b7c473208d25a4c0ed5a","last_reissued_at":"2026-05-18T01:49:24.643273Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:49:24.643273Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Correlation Functions of the SU(infinity) Principal Chiral Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-lat","nlin.SI"],"primary_cat":"hep-th","authors_text":"Axel Cortes Cubero, Peter Orland","submitted_at":"2013-06-08T15:25:52Z","abstract_excerpt":"We obtain exact matrix elements of physical operators of the (1+1)-dimensional nonlinear sigma model of an SU(N)-valued bare field, in the 't Hooft limit N goes to infinity. Specifically, all the form factors of the Noether current and the stress-energy-momentum tensor are found with an integrable bootstrap method. These form factors are used to find vacuum expectation values of products of these operators."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.1930","kind":"arxiv","version":4},"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":"1306.1930","created_at":"2026-05-18T01:49:24.643433+00:00"},{"alias_kind":"arxiv_version","alias_value":"1306.1930v4","created_at":"2026-05-18T01:49:24.643433+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.1930","created_at":"2026-05-18T01:49:24.643433+00:00"},{"alias_kind":"pith_short_12","alias_value":"NOFDPQXFANKZ","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_16","alias_value":"NOFDPQXFANKZDDJK","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_8","alias_value":"NOFDPQXF","created_at":"2026-05-18T12:27:52.871228+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/NOFDPQXFANKZDDJK6TCTCUS6H6","json":"https://pith.science/pith/NOFDPQXFANKZDDJK6TCTCUS6H6.json","graph_json":"https://pith.science/api/pith-number/NOFDPQXFANKZDDJK6TCTCUS6H6/graph.json","events_json":"https://pith.science/api/pith-number/NOFDPQXFANKZDDJK6TCTCUS6H6/events.json","paper":"https://pith.science/paper/NOFDPQXF"},"agent_actions":{"view_html":"https://pith.science/pith/NOFDPQXFANKZDDJK6TCTCUS6H6","download_json":"https://pith.science/pith/NOFDPQXFANKZDDJK6TCTCUS6H6.json","view_paper":"https://pith.science/paper/NOFDPQXF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1306.1930&json=true","fetch_graph":"https://pith.science/api/pith-number/NOFDPQXFANKZDDJK6TCTCUS6H6/graph.json","fetch_events":"https://pith.science/api/pith-number/NOFDPQXFANKZDDJK6TCTCUS6H6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NOFDPQXFANKZDDJK6TCTCUS6H6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NOFDPQXFANKZDDJK6TCTCUS6H6/action/storage_attestation","attest_author":"https://pith.science/pith/NOFDPQXFANKZDDJK6TCTCUS6H6/action/author_attestation","sign_citation":"https://pith.science/pith/NOFDPQXFANKZDDJK6TCTCUS6H6/action/citation_signature","submit_replication":"https://pith.science/pith/NOFDPQXFANKZDDJK6TCTCUS6H6/action/replication_record"}},"created_at":"2026-05-18T01:49:24.643433+00:00","updated_at":"2026-05-18T01:49:24.643433+00:00"}