{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:JBBPO3JCH4JLARNFSQSCUSIGOF","short_pith_number":"pith:JBBPO3JC","schema_version":"1.0","canonical_sha256":"4842f76d223f12b045a594242a49067172556a6ec3875b1f4ffa0b8578746a72","source":{"kind":"arxiv","id":"2404.13373","version":1},"attestation_state":"computed","paper":{"title":"Phenomenology of 3-3-1 models with radiative inverse seesaw mechanism","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. E. C\\'arcamo Hern\\'andez, Cesar Bonilla, D. T. Huong, H. N. Long, Iv\\'an Schmidt, P. N. Thu, V. H. Binh, Vishnudath K. N.","submitted_at":"2024-04-20T13:20:25Z","abstract_excerpt":"We propose two models based on the $SU(3)_C \\times SU(3)_L \\times U(1)_X$ gauge symmetry, each incorporating distinct inverse seesaw mechanisms for generating neutrino masses at the radiative level. Therefore, neutrino masses are suppressed by the radiative nature of the mass generation mechanism, which occurs after the spontaneous breaking of the global lepton number symmetry. Both scenarios discussed here are characterized by the presence of vector-like charged leptons, which are involved in generating the masses of the Standard Model charged leptons. These additional vector-like fermions co"},"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":"2404.13373","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-20T13:20:25Z","cross_cats_sorted":[],"title_canon_sha256":"2957d6233bc2e884121765e8365026298ce11539a7e82887f3786bf8a53cc3ad","abstract_canon_sha256":"62ea13721fa8229e2ae973218b8c44618ecfe538c06533cc21f6db61cf89ab4d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:27:53.721373Z","signature_b64":"4409UhMswO/o95PvnmMlRwGgh4MjDrdJfMD2SzzNjqOoN6MFLBTkikvXGne0/9TXbU7+CB4pIEDcW+vB3syOBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4842f76d223f12b045a594242a49067172556a6ec3875b1f4ffa0b8578746a72","last_reissued_at":"2026-07-05T09:27:53.720850Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:27:53.720850Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phenomenology of 3-3-1 models with radiative inverse seesaw mechanism","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. E. C\\'arcamo Hern\\'andez, Cesar Bonilla, D. T. Huong, H. N. Long, Iv\\'an Schmidt, P. N. Thu, V. H. Binh, Vishnudath K. N.","submitted_at":"2024-04-20T13:20:25Z","abstract_excerpt":"We propose two models based on the $SU(3)_C \\times SU(3)_L \\times U(1)_X$ gauge symmetry, each incorporating distinct inverse seesaw mechanisms for generating neutrino masses at the radiative level. Therefore, neutrino masses are suppressed by the radiative nature of the mass generation mechanism, which occurs after the spontaneous breaking of the global lepton number symmetry. Both scenarios discussed here are characterized by the presence of vector-like charged leptons, which are involved in generating the masses of the Standard Model charged leptons. These additional vector-like fermions co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.13373","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2404.13373/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":"2404.13373","created_at":"2026-07-05T09:27:53.720912+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.13373v1","created_at":"2026-07-05T09:27:53.720912+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.13373","created_at":"2026-07-05T09:27:53.720912+00:00"},{"alias_kind":"pith_short_12","alias_value":"JBBPO3JCH4JL","created_at":"2026-07-05T09:27:53.720912+00:00"},{"alias_kind":"pith_short_16","alias_value":"JBBPO3JCH4JLARNF","created_at":"2026-07-05T09:27:53.720912+00:00"},{"alias_kind":"pith_short_8","alias_value":"JBBPO3JC","created_at":"2026-07-05T09:27:53.720912+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":52,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JBBPO3JCH4JLARNFSQSCUSIGOF","json":"https://pith.science/pith/JBBPO3JCH4JLARNFSQSCUSIGOF.json","graph_json":"https://pith.science/api/pith-number/JBBPO3JCH4JLARNFSQSCUSIGOF/graph.json","events_json":"https://pith.science/api/pith-number/JBBPO3JCH4JLARNFSQSCUSIGOF/events.json","paper":"https://pith.science/paper/JBBPO3JC"},"agent_actions":{"view_html":"https://pith.science/pith/JBBPO3JCH4JLARNFSQSCUSIGOF","download_json":"https://pith.science/pith/JBBPO3JCH4JLARNFSQSCUSIGOF.json","view_paper":"https://pith.science/paper/JBBPO3JC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.13373&json=true","fetch_graph":"https://pith.science/api/pith-number/JBBPO3JCH4JLARNFSQSCUSIGOF/graph.json","fetch_events":"https://pith.science/api/pith-number/JBBPO3JCH4JLARNFSQSCUSIGOF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JBBPO3JCH4JLARNFSQSCUSIGOF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JBBPO3JCH4JLARNFSQSCUSIGOF/action/storage_attestation","attest_author":"https://pith.science/pith/JBBPO3JCH4JLARNFSQSCUSIGOF/action/author_attestation","sign_citation":"https://pith.science/pith/JBBPO3JCH4JLARNFSQSCUSIGOF/action/citation_signature","submit_replication":"https://pith.science/pith/JBBPO3JCH4JLARNFSQSCUSIGOF/action/replication_record"}},"created_at":"2026-07-05T09:27:53.720912+00:00","updated_at":"2026-07-05T09:27:53.720912+00:00"}