{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:CTPG4N46BWXSPMXOHORFRUYNXT","short_pith_number":"pith:CTPG4N46","schema_version":"1.0","canonical_sha256":"14de6e379e0daf27b2ee3ba258d30dbcf8cce772ab56d2936d1f477bfb4fcbfe","source":{"kind":"arxiv","id":"2405.18017","version":3},"attestation_state":"computed","paper":{"title":"Threshold Effects on the Massless Neutrino in the Canonical Seesaw Mechanism","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Di Zhang","submitted_at":"2024-05-28T09:59:08Z","abstract_excerpt":"In this work, we revisit the one-loop renormalization group equations (RGEs) among non-degenerate seesaw scales, i.e., threshold effects in the canonical seesaw mechanism, which have been obtained for more than two decades. Different from the previous work only focusing on the Weinberg operator, we derive the complete one-loop RGEs of all three dimension-five operators in the Standard Model effective field theory with right-handed neutrinos ($\\nu$SMEFT) and apply them to threshold effects in the canonical seesaw mechanism. We find some contributions from the Weinberg operator to its Wilson coe"},"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":"2405.18017","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-05-28T09:59:08Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"9e38ff6e17a35ef42cd961c2b06cdf7199d222d7bf12ec8844a098f8766d1c54","abstract_canon_sha256":"69778e4572556f6c71a5a2d612c66d56e56124e67a31a19608b72a300d3b31ee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:42:35.215389Z","signature_b64":"RHGu4XtArZn+3GR88kiGXdtI5rmSgXCvQZoT+1lvbK158RIJxO2dGBN9ixXdDLakoRB24kk70Xu8RNsLkrtVCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"14de6e379e0daf27b2ee3ba258d30dbcf8cce772ab56d2936d1f477bfb4fcbfe","last_reissued_at":"2026-07-05T10:42:35.214891Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:42:35.214891Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Threshold Effects on the Massless Neutrino in the Canonical Seesaw Mechanism","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Di Zhang","submitted_at":"2024-05-28T09:59:08Z","abstract_excerpt":"In this work, we revisit the one-loop renormalization group equations (RGEs) among non-degenerate seesaw scales, i.e., threshold effects in the canonical seesaw mechanism, which have been obtained for more than two decades. Different from the previous work only focusing on the Weinberg operator, we derive the complete one-loop RGEs of all three dimension-five operators in the Standard Model effective field theory with right-handed neutrinos ($\\nu$SMEFT) and apply them to threshold effects in the canonical seesaw mechanism. We find some contributions from the Weinberg operator to its Wilson coe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.18017","kind":"arxiv","version":3},"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/2405.18017/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":"2405.18017","created_at":"2026-07-05T10:42:35.214944+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.18017v3","created_at":"2026-07-05T10:42:35.214944+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.18017","created_at":"2026-07-05T10:42:35.214944+00:00"},{"alias_kind":"pith_short_12","alias_value":"CTPG4N46BWXS","created_at":"2026-07-05T10:42:35.214944+00:00"},{"alias_kind":"pith_short_16","alias_value":"CTPG4N46BWXSPMXO","created_at":"2026-07-05T10:42:35.214944+00:00"},{"alias_kind":"pith_short_8","alias_value":"CTPG4N46","created_at":"2026-07-05T10:42:35.214944+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2511.08679","citing_title":"Hunting for Neutrino Texture Zeros with Muon and Tau Flavor Violation","ref_index":112,"is_internal_anchor":false},{"citing_arxiv_id":"2601.02452","citing_title":"Fixed points of the renormalisation group running of quark and fermion mixing matrices in the Standard Model and beyond","ref_index":16,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CTPG4N46BWXSPMXOHORFRUYNXT","json":"https://pith.science/pith/CTPG4N46BWXSPMXOHORFRUYNXT.json","graph_json":"https://pith.science/api/pith-number/CTPG4N46BWXSPMXOHORFRUYNXT/graph.json","events_json":"https://pith.science/api/pith-number/CTPG4N46BWXSPMXOHORFRUYNXT/events.json","paper":"https://pith.science/paper/CTPG4N46"},"agent_actions":{"view_html":"https://pith.science/pith/CTPG4N46BWXSPMXOHORFRUYNXT","download_json":"https://pith.science/pith/CTPG4N46BWXSPMXOHORFRUYNXT.json","view_paper":"https://pith.science/paper/CTPG4N46","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.18017&json=true","fetch_graph":"https://pith.science/api/pith-number/CTPG4N46BWXSPMXOHORFRUYNXT/graph.json","fetch_events":"https://pith.science/api/pith-number/CTPG4N46BWXSPMXOHORFRUYNXT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CTPG4N46BWXSPMXOHORFRUYNXT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CTPG4N46BWXSPMXOHORFRUYNXT/action/storage_attestation","attest_author":"https://pith.science/pith/CTPG4N46BWXSPMXOHORFRUYNXT/action/author_attestation","sign_citation":"https://pith.science/pith/CTPG4N46BWXSPMXOHORFRUYNXT/action/citation_signature","submit_replication":"https://pith.science/pith/CTPG4N46BWXSPMXOHORFRUYNXT/action/replication_record"}},"created_at":"2026-07-05T10:42:35.214944+00:00","updated_at":"2026-07-05T10:42:35.214944+00:00"}