{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:EI7DB6AIBHTOCDPUDRCLWDEARY","short_pith_number":"pith:EI7DB6AI","schema_version":"1.0","canonical_sha256":"223e30f80809e6e10df41c44bb0c808e391983869e2b19e1f8ca26b61b0ac595","source":{"kind":"arxiv","id":"1907.04042","version":2},"attestation_state":"computed","paper":{"title":"Predictions for the neutrino parameters in the minimal model extended by linear combination of U(1)$_{L_e-L_\\mu}$, U(1)$_{L_\\mu-L_\\tau}$ and U(1)$_{B-L}$ gauge symmetries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Kento Asai","submitted_at":"2019-07-09T08:32:58Z","abstract_excerpt":"We study the minimal extensions of the Standard Model by a linear combination of U(1)$_{L_e-L_\\mu}$, U(1)$_{L_\\mu-L_\\tau}$ and U(1)$_{B-L}$ gauge symmetries, where three right-handed neutrinos and one U(1)-breaking SU(2)$_L$ singlet or doublet scalar are introduced. Because of the dependence on the lepton flavor, the structures of both Dirac and Majorana mass matrices of neutrinos are restricted. In particular, the two-zero minor and texture structures in the mass matrix for the active neutrinos are interesting. Analyzing these structures, we obtain uniquely all the neutrino parameters, namely"},"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":"1907.04042","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-07-09T08:32:58Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"b383f106ea27b2144b3f3e205c3851f6eac3ac10e3997c4827d9cb35d70ed35a","abstract_canon_sha256":"d53514442211a933c3c3624f6802486d1afb48949a8a404fb8f5930174f303e4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:13:06.073765Z","signature_b64":"iXhPwXw2NBjWVgpupU1FUzkpzqtQeY+PL28OolgvVl6aHrD69LYQN6BADQ5eDuy4zDMTIVLehhcevHXUVKkcBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"223e30f80809e6e10df41c44bb0c808e391983869e2b19e1f8ca26b61b0ac595","last_reissued_at":"2026-07-05T01:13:06.073280Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:13:06.073280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Predictions for the neutrino parameters in the minimal model extended by linear combination of U(1)$_{L_e-L_\\mu}$, U(1)$_{L_\\mu-L_\\tau}$ and U(1)$_{B-L}$ gauge symmetries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Kento Asai","submitted_at":"2019-07-09T08:32:58Z","abstract_excerpt":"We study the minimal extensions of the Standard Model by a linear combination of U(1)$_{L_e-L_\\mu}$, U(1)$_{L_\\mu-L_\\tau}$ and U(1)$_{B-L}$ gauge symmetries, where three right-handed neutrinos and one U(1)-breaking SU(2)$_L$ singlet or doublet scalar are introduced. Because of the dependence on the lepton flavor, the structures of both Dirac and Majorana mass matrices of neutrinos are restricted. In particular, the two-zero minor and texture structures in the mass matrix for the active neutrinos are interesting. Analyzing these structures, we obtain uniquely all the neutrino parameters, namely"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1907.04042","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/1907.04042/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":"1907.04042","created_at":"2026-07-05T01:13:06.073339+00:00"},{"alias_kind":"arxiv_version","alias_value":"1907.04042v2","created_at":"2026-07-05T01:13:06.073339+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1907.04042","created_at":"2026-07-05T01:13:06.073339+00:00"},{"alias_kind":"pith_short_12","alias_value":"EI7DB6AIBHTO","created_at":"2026-07-05T01:13:06.073339+00:00"},{"alias_kind":"pith_short_16","alias_value":"EI7DB6AIBHTOCDPU","created_at":"2026-07-05T01:13:06.073339+00:00"},{"alias_kind":"pith_short_8","alias_value":"EI7DB6AI","created_at":"2026-07-05T01:13:06.073339+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.08384","citing_title":"Revisiting One-Zero and Two-Zero Neutrino Mass Textures in Light of Recent Oscillation and Cosmological Data","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2407.20615","citing_title":"Prospects of five-dimensional $L_\\mu-L_\\tau$ gauge interactions in the light of elastic neutrino-electron scatterings: The scope of the DUNE near detector","ref_index":9,"is_internal_anchor":false},{"citing_arxiv_id":"2510.25613","citing_title":"Muon Beam Dump Experiments explicate five-dimensional nature of $U(1)_{L_{\\mu}-L_{\\tau}}$","ref_index":55,"is_internal_anchor":false},{"citing_arxiv_id":"2604.05041","citing_title":"Aspects of a Five-Dimensional $U(1)_{L_\\mu - L_\\tau}$ Model at Future Muon-Based Colliders","ref_index":11,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EI7DB6AIBHTOCDPUDRCLWDEARY","json":"https://pith.science/pith/EI7DB6AIBHTOCDPUDRCLWDEARY.json","graph_json":"https://pith.science/api/pith-number/EI7DB6AIBHTOCDPUDRCLWDEARY/graph.json","events_json":"https://pith.science/api/pith-number/EI7DB6AIBHTOCDPUDRCLWDEARY/events.json","paper":"https://pith.science/paper/EI7DB6AI"},"agent_actions":{"view_html":"https://pith.science/pith/EI7DB6AIBHTOCDPUDRCLWDEARY","download_json":"https://pith.science/pith/EI7DB6AIBHTOCDPUDRCLWDEARY.json","view_paper":"https://pith.science/paper/EI7DB6AI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1907.04042&json=true","fetch_graph":"https://pith.science/api/pith-number/EI7DB6AIBHTOCDPUDRCLWDEARY/graph.json","fetch_events":"https://pith.science/api/pith-number/EI7DB6AIBHTOCDPUDRCLWDEARY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EI7DB6AIBHTOCDPUDRCLWDEARY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EI7DB6AIBHTOCDPUDRCLWDEARY/action/storage_attestation","attest_author":"https://pith.science/pith/EI7DB6AIBHTOCDPUDRCLWDEARY/action/author_attestation","sign_citation":"https://pith.science/pith/EI7DB6AIBHTOCDPUDRCLWDEARY/action/citation_signature","submit_replication":"https://pith.science/pith/EI7DB6AIBHTOCDPUDRCLWDEARY/action/replication_record"}},"created_at":"2026-07-05T01:13:06.073339+00:00","updated_at":"2026-07-05T01:13:06.073339+00:00"}