{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:MLW5XMO42H5WS3NOMQKYBMRB2Y","short_pith_number":"pith:MLW5XMO4","schema_version":"1.0","canonical_sha256":"62eddbb1dcd1fb696dae641580b221d603b56748b7880951902c8caf767e675f","source":{"kind":"arxiv","id":"hep-th/9603190","version":1},"attestation_state":"computed","paper":{"title":"Exact Scattering in the SU(n) Supersymmetric Principal Chiral Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jonathan M. Evans, Timothy J. Hollowood","submitted_at":"1996-03-28T17:44:58Z","abstract_excerpt":"The complete spectrum of states in the supersymmetric principal chiral model based on SU(n) is conjectured, and an exact factorizable S-matrix is proposed to describe scattering amongst these states. The SU(n)_L*SU(n)_R symmetry of the lagrangian is manifest in the S-matrix construction. The supersymmetries, on the other hand, are incorporated in the guise of spin-1/2 charges acting on a set of RSOS kinks associated with su(n) at level n. To test the proposed S-matrix, calculations of the change in the ground-state energy in the presence of a coupling to a background charge are carried out. Th"},"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":"hep-th/9603190","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-03-28T17:44:58Z","cross_cats_sorted":[],"title_canon_sha256":"19f375eb8b56186fd6d040300d7a8fb6df0e324cd674815325314d8436e4614c","abstract_canon_sha256":"05e9c67cce8adfea2e08135a6474013cc2dc7526596f5b8722dcece4f76b40e2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:02:06.361326Z","signature_b64":"IrMC+9nm0Y3TS1dqh31Rzd6n7oMIDYkp1I0/maH9liREkKXvPD+vpxT87G78Jca3+9fIYFWH9+6Yt/AvpiJzAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"62eddbb1dcd1fb696dae641580b221d603b56748b7880951902c8caf767e675f","last_reissued_at":"2026-07-04T16:02:06.360965Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:02:06.360965Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exact Scattering in the SU(n) Supersymmetric Principal Chiral Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jonathan M. Evans, Timothy J. Hollowood","submitted_at":"1996-03-28T17:44:58Z","abstract_excerpt":"The complete spectrum of states in the supersymmetric principal chiral model based on SU(n) is conjectured, and an exact factorizable S-matrix is proposed to describe scattering amongst these states. The SU(n)_L*SU(n)_R symmetry of the lagrangian is manifest in the S-matrix construction. The supersymmetries, on the other hand, are incorporated in the guise of spin-1/2 charges acting on a set of RSOS kinks associated with su(n) at level n. To test the proposed S-matrix, calculations of the change in the ground-state energy in the presence of a coupling to a background charge are carried out. Th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9603190","kind":"arxiv","version":1},"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/hep-th/9603190/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":"hep-th/9603190","created_at":"2026-07-04T16:02:06.361028+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9603190v1","created_at":"2026-07-04T16:02:06.361028+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9603190","created_at":"2026-07-04T16:02:06.361028+00:00"},{"alias_kind":"pith_short_12","alias_value":"MLW5XMO42H5W","created_at":"2026-07-04T16:02:06.361028+00:00"},{"alias_kind":"pith_short_16","alias_value":"MLW5XMO42H5WS3NO","created_at":"2026-07-04T16:02:06.361028+00:00"},{"alias_kind":"pith_short_8","alias_value":"MLW5XMO4","created_at":"2026-07-04T16:02:06.361028+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.16435","citing_title":"The complete trans-series for conserved charges in integrable field theories","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MLW5XMO42H5WS3NOMQKYBMRB2Y","json":"https://pith.science/pith/MLW5XMO42H5WS3NOMQKYBMRB2Y.json","graph_json":"https://pith.science/api/pith-number/MLW5XMO42H5WS3NOMQKYBMRB2Y/graph.json","events_json":"https://pith.science/api/pith-number/MLW5XMO42H5WS3NOMQKYBMRB2Y/events.json","paper":"https://pith.science/paper/MLW5XMO4"},"agent_actions":{"view_html":"https://pith.science/pith/MLW5XMO42H5WS3NOMQKYBMRB2Y","download_json":"https://pith.science/pith/MLW5XMO42H5WS3NOMQKYBMRB2Y.json","view_paper":"https://pith.science/paper/MLW5XMO4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9603190&json=true","fetch_graph":"https://pith.science/api/pith-number/MLW5XMO42H5WS3NOMQKYBMRB2Y/graph.json","fetch_events":"https://pith.science/api/pith-number/MLW5XMO42H5WS3NOMQKYBMRB2Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MLW5XMO42H5WS3NOMQKYBMRB2Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MLW5XMO42H5WS3NOMQKYBMRB2Y/action/storage_attestation","attest_author":"https://pith.science/pith/MLW5XMO42H5WS3NOMQKYBMRB2Y/action/author_attestation","sign_citation":"https://pith.science/pith/MLW5XMO42H5WS3NOMQKYBMRB2Y/action/citation_signature","submit_replication":"https://pith.science/pith/MLW5XMO42H5WS3NOMQKYBMRB2Y/action/replication_record"}},"created_at":"2026-07-04T16:02:06.361028+00:00","updated_at":"2026-07-04T16:02:06.361028+00:00"}