{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:RDTW63BRKDJKZ2UL74WIDLPQWV","short_pith_number":"pith:RDTW63BR","schema_version":"1.0","canonical_sha256":"88e76f6c3150d2acea8bff2c81adf0b54a8edc60ff78b05d2ae3ba71f420ac66","source":{"kind":"arxiv","id":"hep-ph/0106287","version":2},"attestation_state":"computed","paper":{"title":"Indirect Bounds on Z-> mu e and Lepton Flavor Violation at Future Colliders","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David Delepine, Francesco Vissani (INFN, Gran Sasso)","submitted_at":"2001-06-26T13:59:13Z","abstract_excerpt":"Motivated by the interest in lepton number violating processes, we study the connection between the rate of Z -> mu e decay and those of the low-energy processes mu ->3 e, and mu -> e conversion in nuclear field. We show that if the vector or axial Z form factors are dominant, Br(Z->mu e) is not observable, while if the Z dipole form factors are dominant, the relatively weak indirect bound Br(Z->mu e)<7 10^{-9} does not fully preclude a signal at future colliders, as TESLA. We finally comment on the relation of Z->mu e with Z->tau e and Z->tau mu decays, and suggest a simple scaling law for th"},"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":"hep-ph/0106287","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-06-26T13:59:13Z","cross_cats_sorted":[],"title_canon_sha256":"554bd7f7e5474f13cc258bf04bb2092ef090c3400307842b9d41e0b32a741dfd","abstract_canon_sha256":"404fc32b0d9b861c1ea888dce6ddf92e7eb7b4d58b85dfbc138aa1747103d217"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:23.492181Z","signature_b64":"Xu/eb4fz5fl3gyJ3+tRuprcNSiQR9RLzHSEdIH5Arr4e39Rb2g+ReL0c+xvj6tZocn8UOXUwp227rvhoZcr8Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"88e76f6c3150d2acea8bff2c81adf0b54a8edc60ff78b05d2ae3ba71f420ac66","last_reissued_at":"2026-07-04T16:27:23.491847Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:23.491847Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Indirect Bounds on Z-> mu e and Lepton Flavor Violation at Future Colliders","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David Delepine, Francesco Vissani (INFN, Gran Sasso)","submitted_at":"2001-06-26T13:59:13Z","abstract_excerpt":"Motivated by the interest in lepton number violating processes, we study the connection between the rate of Z -> mu e decay and those of the low-energy processes mu ->3 e, and mu -> e conversion in nuclear field. We show that if the vector or axial Z form factors are dominant, Br(Z->mu e) is not observable, while if the Z dipole form factors are dominant, the relatively weak indirect bound Br(Z->mu e)<7 10^{-9} does not fully preclude a signal at future colliders, as TESLA. We finally comment on the relation of Z->mu e with Z->tau e and Z->tau mu decays, and suggest a simple scaling law for th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0106287","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/hep-ph/0106287/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":"hep-ph/0106287","created_at":"2026-07-04T16:27:23.491904+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0106287v2","created_at":"2026-07-04T16:27:23.491904+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0106287","created_at":"2026-07-04T16:27:23.491904+00:00"},{"alias_kind":"pith_short_12","alias_value":"RDTW63BRKDJK","created_at":"2026-07-04T16:27:23.491904+00:00"},{"alias_kind":"pith_short_16","alias_value":"RDTW63BRKDJKZ2UL","created_at":"2026-07-04T16:27:23.491904+00:00"},{"alias_kind":"pith_short_8","alias_value":"RDTW63BR","created_at":"2026-07-04T16:27:23.491904+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.11653","citing_title":"Probing Lepton Flavor Violation at Linear Electron-Positron Colliders","ref_index":11,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RDTW63BRKDJKZ2UL74WIDLPQWV","json":"https://pith.science/pith/RDTW63BRKDJKZ2UL74WIDLPQWV.json","graph_json":"https://pith.science/api/pith-number/RDTW63BRKDJKZ2UL74WIDLPQWV/graph.json","events_json":"https://pith.science/api/pith-number/RDTW63BRKDJKZ2UL74WIDLPQWV/events.json","paper":"https://pith.science/paper/RDTW63BR"},"agent_actions":{"view_html":"https://pith.science/pith/RDTW63BRKDJKZ2UL74WIDLPQWV","download_json":"https://pith.science/pith/RDTW63BRKDJKZ2UL74WIDLPQWV.json","view_paper":"https://pith.science/paper/RDTW63BR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0106287&json=true","fetch_graph":"https://pith.science/api/pith-number/RDTW63BRKDJKZ2UL74WIDLPQWV/graph.json","fetch_events":"https://pith.science/api/pith-number/RDTW63BRKDJKZ2UL74WIDLPQWV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RDTW63BRKDJKZ2UL74WIDLPQWV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RDTW63BRKDJKZ2UL74WIDLPQWV/action/storage_attestation","attest_author":"https://pith.science/pith/RDTW63BRKDJKZ2UL74WIDLPQWV/action/author_attestation","sign_citation":"https://pith.science/pith/RDTW63BRKDJKZ2UL74WIDLPQWV/action/citation_signature","submit_replication":"https://pith.science/pith/RDTW63BRKDJKZ2UL74WIDLPQWV/action/replication_record"}},"created_at":"2026-07-04T16:27:23.491904+00:00","updated_at":"2026-07-04T16:27:23.491904+00:00"}