{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:DPOIZVNDS22UFKRPHHBQA2ZUEM","short_pith_number":"pith:DPOIZVND","schema_version":"1.0","canonical_sha256":"1bdc8cd5a396b542aa2f39c3006b342339eda26796eb504538b004ead5267bca","source":{"kind":"arxiv","id":"hep-th/9702127","version":1},"attestation_state":"computed","paper":{"title":"Quaternionic Electroweak Theory and CKM Matrix","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"INFN, Lecce), Stefano De Leo (Dip. di Fisica","submitted_at":"1997-02-17T10:13:20Z","abstract_excerpt":"We find in our quaternionic version of the electroweak theory an apparently hopeless problem: In going from complex to quaternions, the calculation of the real-valued parameters of the CKM matrix drastically changes. We aim to explain this quaternionic puzzle."},"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/9702127","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1997-02-17T10:13:20Z","cross_cats_sorted":[],"title_canon_sha256":"e22afe01d69acf966f83ace55c3330ba51dbc0529e59e7418a8dd3ad5d3eb464","abstract_canon_sha256":"be06fd3878f5e2758734d57c7875d969c77202741e9ba5358be42ec447ed2b15"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:37.425187Z","signature_b64":"y/z1h9v2b4sWApqIk7CnkgqkVDiHwG+ft6pmSnpqO2fYf4OJtYsLbQsUwbw0L6DyBeYOr8LL/u7ZtF4UQuMGDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1bdc8cd5a396b542aa2f39c3006b342339eda26796eb504538b004ead5267bca","last_reissued_at":"2026-05-18T01:38:37.424482Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:37.424482Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quaternionic Electroweak Theory and CKM Matrix","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"INFN, Lecce), Stefano De Leo (Dip. di Fisica","submitted_at":"1997-02-17T10:13:20Z","abstract_excerpt":"We find in our quaternionic version of the electroweak theory an apparently hopeless problem: In going from complex to quaternions, the calculation of the real-valued parameters of the CKM matrix drastically changes. We aim to explain this quaternionic puzzle."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9702127","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":"hep-th/9702127","created_at":"2026-05-18T01:38:37.424584+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9702127v1","created_at":"2026-05-18T01:38:37.424584+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9702127","created_at":"2026-05-18T01:38:37.424584+00:00"},{"alias_kind":"pith_short_12","alias_value":"DPOIZVNDS22U","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"DPOIZVNDS22UFKRP","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"DPOIZVND","created_at":"2026-05-18T12:25:48.327863+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/DPOIZVNDS22UFKRPHHBQA2ZUEM","json":"https://pith.science/pith/DPOIZVNDS22UFKRPHHBQA2ZUEM.json","graph_json":"https://pith.science/api/pith-number/DPOIZVNDS22UFKRPHHBQA2ZUEM/graph.json","events_json":"https://pith.science/api/pith-number/DPOIZVNDS22UFKRPHHBQA2ZUEM/events.json","paper":"https://pith.science/paper/DPOIZVND"},"agent_actions":{"view_html":"https://pith.science/pith/DPOIZVNDS22UFKRPHHBQA2ZUEM","download_json":"https://pith.science/pith/DPOIZVNDS22UFKRPHHBQA2ZUEM.json","view_paper":"https://pith.science/paper/DPOIZVND","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9702127&json=true","fetch_graph":"https://pith.science/api/pith-number/DPOIZVNDS22UFKRPHHBQA2ZUEM/graph.json","fetch_events":"https://pith.science/api/pith-number/DPOIZVNDS22UFKRPHHBQA2ZUEM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DPOIZVNDS22UFKRPHHBQA2ZUEM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DPOIZVNDS22UFKRPHHBQA2ZUEM/action/storage_attestation","attest_author":"https://pith.science/pith/DPOIZVNDS22UFKRPHHBQA2ZUEM/action/author_attestation","sign_citation":"https://pith.science/pith/DPOIZVNDS22UFKRPHHBQA2ZUEM/action/citation_signature","submit_replication":"https://pith.science/pith/DPOIZVNDS22UFKRPHHBQA2ZUEM/action/replication_record"}},"created_at":"2026-05-18T01:38:37.424584+00:00","updated_at":"2026-05-18T01:38:37.424584+00:00"}