{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:GVVTER2QEWFLLL7A2TEATBE7IQ","short_pith_number":"pith:GVVTER2Q","schema_version":"1.0","canonical_sha256":"356b324750258ab5afe0d4c809849f4418c42ab67322e6ff0dd95ad28e457395","source":{"kind":"arxiv","id":"1408.1518","version":2},"attestation_state":"computed","paper":{"title":"Expectation values of flavor-neutrino numbers with respect to neutrino-source hadron states --Neutrino oscillations and decay probabilities--","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kanji Fujii, Norihito Toyota","submitted_at":"2014-08-07T09:14:10Z","abstract_excerpt":"On the basis of quantum field theory, we consider a unified description of various processes accompanied by neutrinos, namely weak decays and oscillation processes. The structures of the expectation values of flavor-neutrino numbers with respect to neutrino-source hadron state are investigated. Due to the smallness of neutrino masses, we naturally obtain the old (i.e. pre-mixing) formulas of decay probabilities. Together, it is shown that the oscillation formulas, similar to the usual ones, are applied irrespectively of the details of neutrino-producing processes. The derived oscillation formu"},"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":"1408.1518","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-08-07T09:14:10Z","cross_cats_sorted":[],"title_canon_sha256":"438bfb0b5e6e0c02f150c53928e73ba37627f2c6239cbb7c2304e90d260cfcad","abstract_canon_sha256":"e41423913c741b9370dd4bd8de82bfc6d90ca8eeab24b7d14bcd41bddc258719"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:28:05.180620Z","signature_b64":"a2uQsRcdmX0KtrTCCCFKmFmlZCKW2Jen0PreMbn1mECRnVO7YdSpOhPkZeRvNXuxlmUEQiZTkFUMEfYrIkvZBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"356b324750258ab5afe0d4c809849f4418c42ab67322e6ff0dd95ad28e457395","last_reissued_at":"2026-05-18T02:28:05.180196Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:28:05.180196Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Expectation values of flavor-neutrino numbers with respect to neutrino-source hadron states --Neutrino oscillations and decay probabilities--","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kanji Fujii, Norihito Toyota","submitted_at":"2014-08-07T09:14:10Z","abstract_excerpt":"On the basis of quantum field theory, we consider a unified description of various processes accompanied by neutrinos, namely weak decays and oscillation processes. The structures of the expectation values of flavor-neutrino numbers with respect to neutrino-source hadron state are investigated. Due to the smallness of neutrino masses, we naturally obtain the old (i.e. pre-mixing) formulas of decay probabilities. Together, it is shown that the oscillation formulas, similar to the usual ones, are applied irrespectively of the details of neutrino-producing processes. The derived oscillation formu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.1518","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":""},"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":"1408.1518","created_at":"2026-05-18T02:28:05.180271+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.1518v2","created_at":"2026-05-18T02:28:05.180271+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.1518","created_at":"2026-05-18T02:28:05.180271+00:00"},{"alias_kind":"pith_short_12","alias_value":"GVVTER2QEWFL","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_16","alias_value":"GVVTER2QEWFLLL7A","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_8","alias_value":"GVVTER2Q","created_at":"2026-05-18T12:28:30.664211+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/GVVTER2QEWFLLL7A2TEATBE7IQ","json":"https://pith.science/pith/GVVTER2QEWFLLL7A2TEATBE7IQ.json","graph_json":"https://pith.science/api/pith-number/GVVTER2QEWFLLL7A2TEATBE7IQ/graph.json","events_json":"https://pith.science/api/pith-number/GVVTER2QEWFLLL7A2TEATBE7IQ/events.json","paper":"https://pith.science/paper/GVVTER2Q"},"agent_actions":{"view_html":"https://pith.science/pith/GVVTER2QEWFLLL7A2TEATBE7IQ","download_json":"https://pith.science/pith/GVVTER2QEWFLLL7A2TEATBE7IQ.json","view_paper":"https://pith.science/paper/GVVTER2Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.1518&json=true","fetch_graph":"https://pith.science/api/pith-number/GVVTER2QEWFLLL7A2TEATBE7IQ/graph.json","fetch_events":"https://pith.science/api/pith-number/GVVTER2QEWFLLL7A2TEATBE7IQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GVVTER2QEWFLLL7A2TEATBE7IQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GVVTER2QEWFLLL7A2TEATBE7IQ/action/storage_attestation","attest_author":"https://pith.science/pith/GVVTER2QEWFLLL7A2TEATBE7IQ/action/author_attestation","sign_citation":"https://pith.science/pith/GVVTER2QEWFLLL7A2TEATBE7IQ/action/citation_signature","submit_replication":"https://pith.science/pith/GVVTER2QEWFLLL7A2TEATBE7IQ/action/replication_record"}},"created_at":"2026-05-18T02:28:05.180271+00:00","updated_at":"2026-05-18T02:28:05.180271+00:00"}