{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:EIHYHJKAEPO3DFXUII63RSRB4R","short_pith_number":"pith:EIHYHJKA","schema_version":"1.0","canonical_sha256":"220f83a54023ddb196f4423db8ca21e471cd2a48dc59cfc7ac01662ffe7f6db8","source":{"kind":"arxiv","id":"2003.05857","version":2},"attestation_state":"computed","paper":{"title":"Radiative generation of neutrino masses in a 3-3-1 type model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arindam Das, Kazuki Enomoto, Kei Yagyu, Shinya Kanemura","submitted_at":"2020-03-12T15:47:42Z","abstract_excerpt":"A new model for tiny neutrino masses is proposed in the gauge theory of $SU(3)_C \\otimes SU(3)_L \\otimes U(1)_X$, where neutrino masses are generated via the quantum effect of new particles. In this model, the fermion content is taken to be minimal to realize the gauge anomaly cancellation, while the scalar sector is extended from the minimal 3-3-1 model to have an additional $SU(3)_L$ triplet field. After $SU(3)_L\\otimes U(1)_X$ is broken into $SU(2)_L\\otimes U(1)_Y$, the \"Zee model\" like diagrams are naturally induced, which contain sufficient lepton flavor violating interactions to reproduc"},"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":"2003.05857","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-03-12T15:47:42Z","cross_cats_sorted":[],"title_canon_sha256":"60fb9e824a7826999c5bde89279dcfd6a47b6e0b29b4a7a5754a6e195c932b35","abstract_canon_sha256":"2f8ef05c6dc5ab8012230306bb68427dba6ec97c418e02db37e1258e804d3681"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:02:45.758464Z","signature_b64":"cYKj4b7Mr+fKtlBun2QYLJLUxvaIH938rgf0XfqsC7Ay1ngWo+zq+r8ODqrhYjf0rHurzHF4cSWm6XthSDT2AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"220f83a54023ddb196f4423db8ca21e471cd2a48dc59cfc7ac01662ffe7f6db8","last_reissued_at":"2026-07-05T01:02:45.758075Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:02:45.758075Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Radiative generation of neutrino masses in a 3-3-1 type model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arindam Das, Kazuki Enomoto, Kei Yagyu, Shinya Kanemura","submitted_at":"2020-03-12T15:47:42Z","abstract_excerpt":"A new model for tiny neutrino masses is proposed in the gauge theory of $SU(3)_C \\otimes SU(3)_L \\otimes U(1)_X$, where neutrino masses are generated via the quantum effect of new particles. In this model, the fermion content is taken to be minimal to realize the gauge anomaly cancellation, while the scalar sector is extended from the minimal 3-3-1 model to have an additional $SU(3)_L$ triplet field. After $SU(3)_L\\otimes U(1)_X$ is broken into $SU(2)_L\\otimes U(1)_Y$, the \"Zee model\" like diagrams are naturally induced, which contain sufficient lepton flavor violating interactions to reproduc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2003.05857","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/2003.05857/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":"2003.05857","created_at":"2026-07-05T01:02:45.758135+00:00"},{"alias_kind":"arxiv_version","alias_value":"2003.05857v2","created_at":"2026-07-05T01:02:45.758135+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2003.05857","created_at":"2026-07-05T01:02:45.758135+00:00"},{"alias_kind":"pith_short_12","alias_value":"EIHYHJKAEPO3","created_at":"2026-07-05T01:02:45.758135+00:00"},{"alias_kind":"pith_short_16","alias_value":"EIHYHJKAEPO3DFXU","created_at":"2026-07-05T01:02:45.758135+00:00"},{"alias_kind":"pith_short_8","alias_value":"EIHYHJKA","created_at":"2026-07-05T01:02:45.758135+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":51,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EIHYHJKAEPO3DFXUII63RSRB4R","json":"https://pith.science/pith/EIHYHJKAEPO3DFXUII63RSRB4R.json","graph_json":"https://pith.science/api/pith-number/EIHYHJKAEPO3DFXUII63RSRB4R/graph.json","events_json":"https://pith.science/api/pith-number/EIHYHJKAEPO3DFXUII63RSRB4R/events.json","paper":"https://pith.science/paper/EIHYHJKA"},"agent_actions":{"view_html":"https://pith.science/pith/EIHYHJKAEPO3DFXUII63RSRB4R","download_json":"https://pith.science/pith/EIHYHJKAEPO3DFXUII63RSRB4R.json","view_paper":"https://pith.science/paper/EIHYHJKA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2003.05857&json=true","fetch_graph":"https://pith.science/api/pith-number/EIHYHJKAEPO3DFXUII63RSRB4R/graph.json","fetch_events":"https://pith.science/api/pith-number/EIHYHJKAEPO3DFXUII63RSRB4R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EIHYHJKAEPO3DFXUII63RSRB4R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EIHYHJKAEPO3DFXUII63RSRB4R/action/storage_attestation","attest_author":"https://pith.science/pith/EIHYHJKAEPO3DFXUII63RSRB4R/action/author_attestation","sign_citation":"https://pith.science/pith/EIHYHJKAEPO3DFXUII63RSRB4R/action/citation_signature","submit_replication":"https://pith.science/pith/EIHYHJKAEPO3DFXUII63RSRB4R/action/replication_record"}},"created_at":"2026-07-05T01:02:45.758135+00:00","updated_at":"2026-07-05T01:02:45.758135+00:00"}