{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:54ZEY7AWKZORPC3TVV7J2I5UVP","short_pith_number":"pith:54ZEY7AW","schema_version":"1.0","canonical_sha256":"ef324c7c16565d178b73ad7e9d23b4abe884a821cc614ccabe050250cf1fcce8","source":{"kind":"arxiv","id":"2401.06214","version":1},"attestation_state":"computed","paper":{"title":"Constraining New Physics models from $\\mu\\to e$ observables in bottom-up EFT","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Marco Ardu, Sacha Davidson, St\\'ephane Lavignac","submitted_at":"2024-01-11T19:00:02Z","abstract_excerpt":"Upcoming experiments will improve the sensitivity to $\\mu\\to e$ processes by several orders of magnitude, and could observe lepton flavour-changing contact interactions for the first time. In this paper, we investigate what could be learned about New Physics from the measurements of these $\\mu\\to e$ observables, using a bottom-up effective field theory (EFT) approach and focusing on three popular models with new particles around the TeV scale (the type II seesaw, the inverse seesaw and a scalar leptoquark). We showed in a previous publication that $\\mu\\to e$ observables have the ability to rul"},"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":"2401.06214","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-01-11T19:00:02Z","cross_cats_sorted":[],"title_canon_sha256":"f42eb59428abcbcc4d0d9307eef5effa743e2e5c5b0437218e0257e3cf3bde73","abstract_canon_sha256":"9828da7c653e6dafef92ee44e84e53ba018e332785a1ce89748a37392326f997"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:32:47.341051Z","signature_b64":"7PaGhr8PNakT957djCWX0ZKJFXIh2HTReAfdxCyulY7ALcJIns1vzDFqdjPEN6uyXXLuEGkcLhWMHx0KR6GhDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef324c7c16565d178b73ad7e9d23b4abe884a821cc614ccabe050250cf1fcce8","last_reissued_at":"2026-07-05T07:32:47.340511Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:32:47.340511Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constraining New Physics models from $\\mu\\to e$ observables in bottom-up EFT","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Marco Ardu, Sacha Davidson, St\\'ephane Lavignac","submitted_at":"2024-01-11T19:00:02Z","abstract_excerpt":"Upcoming experiments will improve the sensitivity to $\\mu\\to e$ processes by several orders of magnitude, and could observe lepton flavour-changing contact interactions for the first time. In this paper, we investigate what could be learned about New Physics from the measurements of these $\\mu\\to e$ observables, using a bottom-up effective field theory (EFT) approach and focusing on three popular models with new particles around the TeV scale (the type II seesaw, the inverse seesaw and a scalar leptoquark). We showed in a previous publication that $\\mu\\to e$ observables have the ability to rul"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.06214","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2401.06214/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":"2401.06214","created_at":"2026-07-05T07:32:47.340572+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.06214v1","created_at":"2026-07-05T07:32:47.340572+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.06214","created_at":"2026-07-05T07:32:47.340572+00:00"},{"alias_kind":"pith_short_12","alias_value":"54ZEY7AWKZOR","created_at":"2026-07-05T07:32:47.340572+00:00"},{"alias_kind":"pith_short_16","alias_value":"54ZEY7AWKZORPC3T","created_at":"2026-07-05T07:32:47.340572+00:00"},{"alias_kind":"pith_short_8","alias_value":"54ZEY7AW","created_at":"2026-07-05T07:32:47.340572+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.02709","citing_title":"Anatomy and Phenomenology of Minimal Flavor Deconstruction in the Lepton Sector","ref_index":70,"is_internal_anchor":false},{"citing_arxiv_id":"2605.20058","citing_title":"Renormalisation and invariants for two U(1)s","ref_index":56,"is_internal_anchor":false},{"citing_arxiv_id":"2507.18236","citing_title":"Search for the lepton-flavor-violating $\\tau^{-} \\rightarrow e^{\\mp} \\ell^{\\pm} \\ell^{\\mp}$ decays at Belle II","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2511.08679","citing_title":"Hunting for Neutrino Texture Zeros with Muon and Tau Flavor Violation","ref_index":83,"is_internal_anchor":false},{"citing_arxiv_id":"2601.18237","citing_title":"Revisiting $\\mu$-$e$ conversion in $R$-parity violating SUSY","ref_index":68,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/54ZEY7AWKZORPC3TVV7J2I5UVP","json":"https://pith.science/pith/54ZEY7AWKZORPC3TVV7J2I5UVP.json","graph_json":"https://pith.science/api/pith-number/54ZEY7AWKZORPC3TVV7J2I5UVP/graph.json","events_json":"https://pith.science/api/pith-number/54ZEY7AWKZORPC3TVV7J2I5UVP/events.json","paper":"https://pith.science/paper/54ZEY7AW"},"agent_actions":{"view_html":"https://pith.science/pith/54ZEY7AWKZORPC3TVV7J2I5UVP","download_json":"https://pith.science/pith/54ZEY7AWKZORPC3TVV7J2I5UVP.json","view_paper":"https://pith.science/paper/54ZEY7AW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.06214&json=true","fetch_graph":"https://pith.science/api/pith-number/54ZEY7AWKZORPC3TVV7J2I5UVP/graph.json","fetch_events":"https://pith.science/api/pith-number/54ZEY7AWKZORPC3TVV7J2I5UVP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/54ZEY7AWKZORPC3TVV7J2I5UVP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/54ZEY7AWKZORPC3TVV7J2I5UVP/action/storage_attestation","attest_author":"https://pith.science/pith/54ZEY7AWKZORPC3TVV7J2I5UVP/action/author_attestation","sign_citation":"https://pith.science/pith/54ZEY7AWKZORPC3TVV7J2I5UVP/action/citation_signature","submit_replication":"https://pith.science/pith/54ZEY7AWKZORPC3TVV7J2I5UVP/action/replication_record"}},"created_at":"2026-07-05T07:32:47.340572+00:00","updated_at":"2026-07-05T07:32:47.340572+00:00"}