{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:7TQLU6B2R6A6KLY54SPZHQX2EE","short_pith_number":"pith:7TQLU6B2","schema_version":"1.0","canonical_sha256":"fce0ba783a8f81e52f1de49f93c2fa2126e32d555b6db67cc24cf840dd484a75","source":{"kind":"arxiv","id":"1405.2368","version":1},"attestation_state":"computed","paper":{"title":"Radiative Generation of Lepton Masses with the $U(1)'$ Gauge Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hiroshi Okada, Kei Yagyu","submitted_at":"2014-05-09T23:20:47Z","abstract_excerpt":"We revisit our previous model proposed in Ref. \\cite{Okada:2013iba}, in which lepton masses except the tauon mass are generated at the one-loop level in a TeV scale physics. Although in the previous work, rather large Yukawa couplings constants; i.e., greater than about 3, are required to reproduce the muon mass, we do not need to introduce such a large but ${\\cal O}$(1) couplings. In our model, masses for neutrinos (charged-leptons) are generated by a dimension five effective operator with two isospin triplet (singlet and doublet) scalar fields. Thus, the mass hierarchy between neutrinos and "},"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":"1405.2368","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-09T23:20:47Z","cross_cats_sorted":[],"title_canon_sha256":"2a408d6f9da289367ceddb43f9755d67918fe005a60586b48494c78c58811e65","abstract_canon_sha256":"5069d57dcf71f275f7ca8ec1ce1e31516f8736f8701dc817045a70d8bd83bc58"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:44:08.899790Z","signature_b64":"Q8EwbulaCKQIDt6OJP/4BR/hFhQ0LlxASRSIEIXSE7goip4OeRh+n5nzUhSasNlv0va0+MP9UaYw0Bp/UofqAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fce0ba783a8f81e52f1de49f93c2fa2126e32d555b6db67cc24cf840dd484a75","last_reissued_at":"2026-05-18T02:44:08.899292Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:44:08.899292Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Radiative Generation of Lepton Masses with the $U(1)'$ Gauge Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hiroshi Okada, Kei Yagyu","submitted_at":"2014-05-09T23:20:47Z","abstract_excerpt":"We revisit our previous model proposed in Ref. \\cite{Okada:2013iba}, in which lepton masses except the tauon mass are generated at the one-loop level in a TeV scale physics. Although in the previous work, rather large Yukawa couplings constants; i.e., greater than about 3, are required to reproduce the muon mass, we do not need to introduce such a large but ${\\cal O}$(1) couplings. In our model, masses for neutrinos (charged-leptons) are generated by a dimension five effective operator with two isospin triplet (singlet and doublet) scalar fields. Thus, the mass hierarchy between neutrinos and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.2368","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":"1405.2368","created_at":"2026-05-18T02:44:08.899372+00:00"},{"alias_kind":"arxiv_version","alias_value":"1405.2368v1","created_at":"2026-05-18T02:44:08.899372+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.2368","created_at":"2026-05-18T02:44:08.899372+00:00"},{"alias_kind":"pith_short_12","alias_value":"7TQLU6B2R6A6","created_at":"2026-05-18T12:28:19.803747+00:00"},{"alias_kind":"pith_short_16","alias_value":"7TQLU6B2R6A6KLY5","created_at":"2026-05-18T12:28:19.803747+00:00"},{"alias_kind":"pith_short_8","alias_value":"7TQLU6B2","created_at":"2026-05-18T12:28:19.803747+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/7TQLU6B2R6A6KLY54SPZHQX2EE","json":"https://pith.science/pith/7TQLU6B2R6A6KLY54SPZHQX2EE.json","graph_json":"https://pith.science/api/pith-number/7TQLU6B2R6A6KLY54SPZHQX2EE/graph.json","events_json":"https://pith.science/api/pith-number/7TQLU6B2R6A6KLY54SPZHQX2EE/events.json","paper":"https://pith.science/paper/7TQLU6B2"},"agent_actions":{"view_html":"https://pith.science/pith/7TQLU6B2R6A6KLY54SPZHQX2EE","download_json":"https://pith.science/pith/7TQLU6B2R6A6KLY54SPZHQX2EE.json","view_paper":"https://pith.science/paper/7TQLU6B2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1405.2368&json=true","fetch_graph":"https://pith.science/api/pith-number/7TQLU6B2R6A6KLY54SPZHQX2EE/graph.json","fetch_events":"https://pith.science/api/pith-number/7TQLU6B2R6A6KLY54SPZHQX2EE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7TQLU6B2R6A6KLY54SPZHQX2EE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7TQLU6B2R6A6KLY54SPZHQX2EE/action/storage_attestation","attest_author":"https://pith.science/pith/7TQLU6B2R6A6KLY54SPZHQX2EE/action/author_attestation","sign_citation":"https://pith.science/pith/7TQLU6B2R6A6KLY54SPZHQX2EE/action/citation_signature","submit_replication":"https://pith.science/pith/7TQLU6B2R6A6KLY54SPZHQX2EE/action/replication_record"}},"created_at":"2026-05-18T02:44:08.899372+00:00","updated_at":"2026-05-18T02:44:08.899372+00:00"}