{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:B35S4PRZK5ZY7AAK6PJBSKPXN7","short_pith_number":"pith:B35S4PRZ","schema_version":"1.0","canonical_sha256":"0efb2e3e3957738f800af3d21929f76fc1f90d5a86ab963ca781771d5e4bf22f","source":{"kind":"arxiv","id":"1611.03409","version":1},"attestation_state":"computed","paper":{"title":"Complementarity in lepton-flavour violating muon decay experiments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Crivellin, A. Signer, G. M. Pruna, S. Davidson","submitted_at":"2016-11-10T17:29:15Z","abstract_excerpt":"This note presents an analysis of lepton-flavour-violating muon decays within the framework of a low-energy effective field theory that contains higher-dimensional operators allowed by QED and QCD symmetries. The decay modes $\\mu\\to e \\gamma$ and $\\mu\\to 3e$ are investigated below the electroweak symmetry-breaking scale, down to energies at which such processes occur, i.e. the muon mass scale. The complete class of dimension-5 and dimension-6 operators is studied systematically at the tree level, and one-loop contributions to the renormalisation group equations are fully taken into account. Cu"},"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":"1611.03409","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-10T17:29:15Z","cross_cats_sorted":[],"title_canon_sha256":"4a9a220a56f0e038ee400252f8867b81d8a4391fe04c16b49ac49fba0ec781d1","abstract_canon_sha256":"932393321fd93b505c22a1730cc523908ca5c66648cc327519a678564cff253d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:43:59.243962Z","signature_b64":"ZXDoLFvUuU8GaMzf591cYWoLCks2LcV8RInugH6rB1cX7RN2C2W1XOC/LDl5Ehz3QDUT8cYIYO/Cqpmv2N1MAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0efb2e3e3957738f800af3d21929f76fc1f90d5a86ab963ca781771d5e4bf22f","last_reissued_at":"2026-05-18T00:43:59.243290Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:43:59.243290Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Complementarity in lepton-flavour violating muon decay experiments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Crivellin, A. Signer, G. M. Pruna, S. Davidson","submitted_at":"2016-11-10T17:29:15Z","abstract_excerpt":"This note presents an analysis of lepton-flavour-violating muon decays within the framework of a low-energy effective field theory that contains higher-dimensional operators allowed by QED and QCD symmetries. The decay modes $\\mu\\to e \\gamma$ and $\\mu\\to 3e$ are investigated below the electroweak symmetry-breaking scale, down to energies at which such processes occur, i.e. the muon mass scale. The complete class of dimension-5 and dimension-6 operators is studied systematically at the tree level, and one-loop contributions to the renormalisation group equations are fully taken into account. Cu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.03409","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":"1611.03409","created_at":"2026-05-18T00:43:59.243412+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.03409v1","created_at":"2026-05-18T00:43:59.243412+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.03409","created_at":"2026-05-18T00:43:59.243412+00:00"},{"alias_kind":"pith_short_12","alias_value":"B35S4PRZK5ZY","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_16","alias_value":"B35S4PRZK5ZY7AAK","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_8","alias_value":"B35S4PRZ","created_at":"2026-05-18T12:30:07.202191+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1906.10483","citing_title":"Lepton Flavour violation in muon decays","ref_index":8,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B35S4PRZK5ZY7AAK6PJBSKPXN7","json":"https://pith.science/pith/B35S4PRZK5ZY7AAK6PJBSKPXN7.json","graph_json":"https://pith.science/api/pith-number/B35S4PRZK5ZY7AAK6PJBSKPXN7/graph.json","events_json":"https://pith.science/api/pith-number/B35S4PRZK5ZY7AAK6PJBSKPXN7/events.json","paper":"https://pith.science/paper/B35S4PRZ"},"agent_actions":{"view_html":"https://pith.science/pith/B35S4PRZK5ZY7AAK6PJBSKPXN7","download_json":"https://pith.science/pith/B35S4PRZK5ZY7AAK6PJBSKPXN7.json","view_paper":"https://pith.science/paper/B35S4PRZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.03409&json=true","fetch_graph":"https://pith.science/api/pith-number/B35S4PRZK5ZY7AAK6PJBSKPXN7/graph.json","fetch_events":"https://pith.science/api/pith-number/B35S4PRZK5ZY7AAK6PJBSKPXN7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B35S4PRZK5ZY7AAK6PJBSKPXN7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B35S4PRZK5ZY7AAK6PJBSKPXN7/action/storage_attestation","attest_author":"https://pith.science/pith/B35S4PRZK5ZY7AAK6PJBSKPXN7/action/author_attestation","sign_citation":"https://pith.science/pith/B35S4PRZK5ZY7AAK6PJBSKPXN7/action/citation_signature","submit_replication":"https://pith.science/pith/B35S4PRZK5ZY7AAK6PJBSKPXN7/action/replication_record"}},"created_at":"2026-05-18T00:43:59.243412+00:00","updated_at":"2026-05-18T00:43:59.243412+00:00"}