{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:SJIZBKQK7TDDTWFETK4GNSJHPG","short_pith_number":"pith:SJIZBKQK","schema_version":"1.0","canonical_sha256":"925190aa0afcc639d8a49ab866c927798857d3e8b6765b5b192598dc838462f2","source":{"kind":"arxiv","id":"1210.3722","version":1},"attestation_state":"computed","paper":{"title":"Z_2-reductions of spinor models in two dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nlin.SI","authors_text":"V. S. Gerdjikov","submitted_at":"2012-10-13T16:56:03Z","abstract_excerpt":"We propose new types of integrable spinor models, generalizing the well known ones of: i) Nambu-Jona-Lasinio-Vaks-Larkin models, related to SU(N); ii) the Gross-Neveu models - SP(2N); and the iii) Zakharov-Mikhailov models - SO(N). We propose a method for constructing their Lax representation and outline the spectral properties of the Lax 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":"1210.3722","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.SI","submitted_at":"2012-10-13T16:56:03Z","cross_cats_sorted":[],"title_canon_sha256":"86f3e0186ea249dc333ecd62df0036b2e0d96fe490ebd661b5aff85a752874b0","abstract_canon_sha256":"85b66a0a176efacd0f8969e42c35fb135726f8f139e88747636869112466ff2f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:43:17.270977Z","signature_b64":"wOMwM9GfGL+hHiLHTvHfu/cQbT08gDTROu1hHUohTau+jLVmGQNjRezX/4TuXzWJlMLbMgAMdZoaGzmtxBkKAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"925190aa0afcc639d8a49ab866c927798857d3e8b6765b5b192598dc838462f2","last_reissued_at":"2026-05-18T03:43:17.270354Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:43:17.270354Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Z_2-reductions of spinor models in two dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nlin.SI","authors_text":"V. S. Gerdjikov","submitted_at":"2012-10-13T16:56:03Z","abstract_excerpt":"We propose new types of integrable spinor models, generalizing the well known ones of: i) Nambu-Jona-Lasinio-Vaks-Larkin models, related to SU(N); ii) the Gross-Neveu models - SP(2N); and the iii) Zakharov-Mikhailov models - SO(N). We propose a method for constructing their Lax representation and outline the spectral properties of the Lax operators."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.3722","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":""},"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":"1210.3722","created_at":"2026-05-18T03:43:17.270442+00:00"},{"alias_kind":"arxiv_version","alias_value":"1210.3722v1","created_at":"2026-05-18T03:43:17.270442+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.3722","created_at":"2026-05-18T03:43:17.270442+00:00"},{"alias_kind":"pith_short_12","alias_value":"SJIZBKQK7TDD","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_16","alias_value":"SJIZBKQK7TDDTWFE","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_8","alias_value":"SJIZBKQK","created_at":"2026-05-18T12:27:20.899486+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/SJIZBKQK7TDDTWFETK4GNSJHPG","json":"https://pith.science/pith/SJIZBKQK7TDDTWFETK4GNSJHPG.json","graph_json":"https://pith.science/api/pith-number/SJIZBKQK7TDDTWFETK4GNSJHPG/graph.json","events_json":"https://pith.science/api/pith-number/SJIZBKQK7TDDTWFETK4GNSJHPG/events.json","paper":"https://pith.science/paper/SJIZBKQK"},"agent_actions":{"view_html":"https://pith.science/pith/SJIZBKQK7TDDTWFETK4GNSJHPG","download_json":"https://pith.science/pith/SJIZBKQK7TDDTWFETK4GNSJHPG.json","view_paper":"https://pith.science/paper/SJIZBKQK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1210.3722&json=true","fetch_graph":"https://pith.science/api/pith-number/SJIZBKQK7TDDTWFETK4GNSJHPG/graph.json","fetch_events":"https://pith.science/api/pith-number/SJIZBKQK7TDDTWFETK4GNSJHPG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SJIZBKQK7TDDTWFETK4GNSJHPG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SJIZBKQK7TDDTWFETK4GNSJHPG/action/storage_attestation","attest_author":"https://pith.science/pith/SJIZBKQK7TDDTWFETK4GNSJHPG/action/author_attestation","sign_citation":"https://pith.science/pith/SJIZBKQK7TDDTWFETK4GNSJHPG/action/citation_signature","submit_replication":"https://pith.science/pith/SJIZBKQK7TDDTWFETK4GNSJHPG/action/replication_record"}},"created_at":"2026-05-18T03:43:17.270442+00:00","updated_at":"2026-05-18T03:43:17.270442+00:00"}