{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q","short_pith_number":"pith:3Z7W2PC4","schema_version":"1.0","canonical_sha256":"de7f6d3c5c2049b0884de3a90ef729e430b121169728f8942b25322ca1b87cba","source":{"kind":"arxiv","id":"hep-ph/9402244","version":1},"attestation_state":"computed","paper":{"title":"A parity invariant $SU(3)_c \\otimes SU(3)_L \\otimes U(1)$ model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"R. Foot","submitted_at":"1994-02-07T23:01:48Z","abstract_excerpt":"We examine a $SU(3)_c \\otimes SU(3)_{L}\\otimes U(1)$ gauge model which has a parity symmetric Lagrangian. The parity symmetry has the novel feature that it interchanges the gluons with the $SU(3)_L$ gauge bosons (which contain the ordinary $SU(2)_L$ weak gauge bosons). We show that the model reduces to the standard model at low energies and also predicts new physics in the form of exotic fermions."},"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-ph/9402244","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-02-07T23:01:48Z","cross_cats_sorted":[],"title_canon_sha256":"570a25e731149e300806bc406266cc5d64a7464fd84ce77c60f21d582aa20d41","abstract_canon_sha256":"09fc2e4dcd382ecb0297d885f4d0b634283b4adc8847a90aa094437a27b6b3f9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:01.546149Z","signature_b64":"FOkfJsu4rqAbGz5W6y+0Yug1v+uQ2Cqc7/cUG+XYY7azyBHEe2fi5G4Ic+V7q9uv+3FY05x6OiYf3n1z6SM5Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"de7f6d3c5c2049b0884de3a90ef729e430b121169728f8942b25322ca1b87cba","last_reissued_at":"2026-05-18T01:39:01.545591Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:01.545591Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A parity invariant $SU(3)_c \\otimes SU(3)_L \\otimes U(1)$ model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"R. Foot","submitted_at":"1994-02-07T23:01:48Z","abstract_excerpt":"We examine a $SU(3)_c \\otimes SU(3)_{L}\\otimes U(1)$ gauge model which has a parity symmetric Lagrangian. The parity symmetry has the novel feature that it interchanges the gluons with the $SU(3)_L$ gauge bosons (which contain the ordinary $SU(2)_L$ weak gauge bosons). We show that the model reduces to the standard model at low energies and also predicts new physics in the form of exotic fermions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9402244","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-ph/9402244","created_at":"2026-05-18T01:39:01.545685+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9402244v1","created_at":"2026-05-18T01:39:01.545685+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9402244","created_at":"2026-05-18T01:39:01.545685+00:00"},{"alias_kind":"pith_short_12","alias_value":"3Z7W2PC4EBE3","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"3Z7W2PC4EBE3BCCN","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"3Z7W2PC4","created_at":"2026-05-18T12:25:47.102015+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/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q","json":"https://pith.science/pith/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q.json","graph_json":"https://pith.science/api/pith-number/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q/graph.json","events_json":"https://pith.science/api/pith-number/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q/events.json","paper":"https://pith.science/paper/3Z7W2PC4"},"agent_actions":{"view_html":"https://pith.science/pith/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q","download_json":"https://pith.science/pith/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q.json","view_paper":"https://pith.science/paper/3Z7W2PC4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9402244&json=true","fetch_graph":"https://pith.science/api/pith-number/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q/graph.json","fetch_events":"https://pith.science/api/pith-number/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q/action/storage_attestation","attest_author":"https://pith.science/pith/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q/action/author_attestation","sign_citation":"https://pith.science/pith/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q/action/citation_signature","submit_replication":"https://pith.science/pith/3Z7W2PC4EBE3BCCN4OUQ55ZJ4Q/action/replication_record"}},"created_at":"2026-05-18T01:39:01.545685+00:00","updated_at":"2026-05-18T01:39:01.545685+00:00"}