{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:KPE3LRYVLHSJTFUQBE7GRRQS2S","short_pith_number":"pith:KPE3LRYV","schema_version":"1.0","canonical_sha256":"53c9b5c71559e4999690093e68c612d4a61af3a4c36c88b63531f12dbb59baa7","source":{"kind":"arxiv","id":"hep-ph/0512096","version":2},"attestation_state":"computed","paper":{"title":"Scalar sextet in the 331 model with right-handed neutrinos","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Nguyen Anh Ky, Nguyen Thi Hong Van","submitted_at":"2005-12-08T10:47:36Z","abstract_excerpt":"A Higgs sextet is introduced in order to generate Dirac and Majorana neutrino masses in the 331 model with right-handed neutrinos. As will be seen, the present sextet introduction leads to a rich neutrino mass structure. The smallness of neutrino masses can be achieved via, for example, a seesaw limit. The fact that the masses of the charged leptons are not effected by their new Yukawa couplings to the sextet is convenient for generating small neutrino masses."},"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/0512096","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-12-08T10:47:36Z","cross_cats_sorted":[],"title_canon_sha256":"0fec98b24aba101823397b3103027cf11258b5a6ff045fe15ea21a5aa8880bb4","abstract_canon_sha256":"546a92a05849ab85bc7ae51d3162d2222e058e2a3c9c6504b13d63c369a06f49"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:55:55.530484Z","signature_b64":"XvMejUIMXm4+SHMtBPZACcPW49GwaT4fg4OVmD0lwVi/wHtXGahz2zMbRiPc8wz6GlpcSGEYPVL8MKMhWNLGAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53c9b5c71559e4999690093e68c612d4a61af3a4c36c88b63531f12dbb59baa7","last_reissued_at":"2026-07-04T16:55:55.530142Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:55:55.530142Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scalar sextet in the 331 model with right-handed neutrinos","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Nguyen Anh Ky, Nguyen Thi Hong Van","submitted_at":"2005-12-08T10:47:36Z","abstract_excerpt":"A Higgs sextet is introduced in order to generate Dirac and Majorana neutrino masses in the 331 model with right-handed neutrinos. As will be seen, the present sextet introduction leads to a rich neutrino mass structure. The smallness of neutrino masses can be achieved via, for example, a seesaw limit. The fact that the masses of the charged leptons are not effected by their new Yukawa couplings to the sextet is convenient for generating small neutrino masses."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0512096","kind":"arxiv","version":2},"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-ph/0512096/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-ph/0512096","created_at":"2026-07-04T16:55:55.530205+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0512096v2","created_at":"2026-07-04T16:55:55.530205+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0512096","created_at":"2026-07-04T16:55:55.530205+00:00"},{"alias_kind":"pith_short_12","alias_value":"KPE3LRYVLHSJ","created_at":"2026-07-04T16:55:55.530205+00:00"},{"alias_kind":"pith_short_16","alias_value":"KPE3LRYVLHSJTFUQ","created_at":"2026-07-04T16:55:55.530205+00:00"},{"alias_kind":"pith_short_8","alias_value":"KPE3LRYV","created_at":"2026-07-04T16:55:55.530205+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.15055","citing_title":"Leptoquark-induced radiative masses for active and sterile neutrinos within the framework of the 3-3-1 model","ref_index":44,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KPE3LRYVLHSJTFUQBE7GRRQS2S","json":"https://pith.science/pith/KPE3LRYVLHSJTFUQBE7GRRQS2S.json","graph_json":"https://pith.science/api/pith-number/KPE3LRYVLHSJTFUQBE7GRRQS2S/graph.json","events_json":"https://pith.science/api/pith-number/KPE3LRYVLHSJTFUQBE7GRRQS2S/events.json","paper":"https://pith.science/paper/KPE3LRYV"},"agent_actions":{"view_html":"https://pith.science/pith/KPE3LRYVLHSJTFUQBE7GRRQS2S","download_json":"https://pith.science/pith/KPE3LRYVLHSJTFUQBE7GRRQS2S.json","view_paper":"https://pith.science/paper/KPE3LRYV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0512096&json=true","fetch_graph":"https://pith.science/api/pith-number/KPE3LRYVLHSJTFUQBE7GRRQS2S/graph.json","fetch_events":"https://pith.science/api/pith-number/KPE3LRYVLHSJTFUQBE7GRRQS2S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KPE3LRYVLHSJTFUQBE7GRRQS2S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KPE3LRYVLHSJTFUQBE7GRRQS2S/action/storage_attestation","attest_author":"https://pith.science/pith/KPE3LRYVLHSJTFUQBE7GRRQS2S/action/author_attestation","sign_citation":"https://pith.science/pith/KPE3LRYVLHSJTFUQBE7GRRQS2S/action/citation_signature","submit_replication":"https://pith.science/pith/KPE3LRYVLHSJTFUQBE7GRRQS2S/action/replication_record"}},"created_at":"2026-07-04T16:55:55.530205+00:00","updated_at":"2026-07-04T16:55:55.530205+00:00"}