{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:J5T5DUEFUBWDOJM2CJROFONIPZ","short_pith_number":"pith:J5T5DUEF","schema_version":"1.0","canonical_sha256":"4f67d1d085a06c37259a1262e2b9a87e6f9b1250dfee9dbda7028dfd26f9e570","source":{"kind":"arxiv","id":"1709.00294","version":2},"attestation_state":"computed","paper":{"title":"Charged Lepton Flavour Violation: An Experimental and Theoretical Introduction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Giovanni Signorelli, Lorenzo Calibbi","submitted_at":"2017-08-31T14:04:37Z","abstract_excerpt":"Charged lepton flavour violating transitions would be a clear signal of new physics beyond the Standard Model. Their search has been carried out in a variety of channels, the most sensitive being those involving a muon: however no positive evidence has been found so far. The MEG experiment has recently set the best limit on such processes by investigating the existence of the $\\mu \\to e\\gamma$ decay. In the next decade several experiments are planned to pursue the search for $\\mu \\to e\\gamma$, $\\mu \\to eee$, $\\mu \\to e$ conversion in nuclei, as well as on processes involving the $\\tau$, to an "},"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":"1709.00294","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-31T14:04:37Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f90baf98090647e4a1b2b3ecbb9fd53d7f3ef5a0f001d866264da17b4fc3a2b1","abstract_canon_sha256":"71db140b0fa783b4f3a8ce83d71000d737e48de348b6b5159657e6bb29edcafe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:35.224971Z","signature_b64":"Z4/B1iPQYwHjezqPFT54Lv/rBunDOp4kJsrN/hGcSXwn0flZ4QqPyd+lrRUgUZ/IulrvNWoIvTyyapQ3UIa2BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f67d1d085a06c37259a1262e2b9a87e6f9b1250dfee9dbda7028dfd26f9e570","last_reissued_at":"2026-05-18T00:24:35.224613Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:35.224613Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charged Lepton Flavour Violation: An Experimental and Theoretical Introduction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Giovanni Signorelli, Lorenzo Calibbi","submitted_at":"2017-08-31T14:04:37Z","abstract_excerpt":"Charged lepton flavour violating transitions would be a clear signal of new physics beyond the Standard Model. Their search has been carried out in a variety of channels, the most sensitive being those involving a muon: however no positive evidence has been found so far. The MEG experiment has recently set the best limit on such processes by investigating the existence of the $\\mu \\to e\\gamma$ decay. In the next decade several experiments are planned to pursue the search for $\\mu \\to e\\gamma$, $\\mu \\to eee$, $\\mu \\to e$ conversion in nuclei, as well as on processes involving the $\\tau$, to an "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.00294","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":"1709.00294","created_at":"2026-05-18T00:24:35.224669+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.00294v2","created_at":"2026-05-18T00:24:35.224669+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.00294","created_at":"2026-05-18T00:24:35.224669+00:00"},{"alias_kind":"pith_short_12","alias_value":"J5T5DUEFUBWD","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_16","alias_value":"J5T5DUEFUBWDOJM2","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_8","alias_value":"J5T5DUEF","created_at":"2026-05-18T12:31:21.493067+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":9,"internal_anchor_count":6,"sample":[{"citing_arxiv_id":"2204.00564","citing_title":"Reach and complementarity of $\\mu\\to e$ searches","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2605.22656","citing_title":"Emergent Neutrino Texture Geometry from Dark Matter and Lepton Flavor Violation in the Scotogenic Model","ref_index":50,"is_internal_anchor":true},{"citing_arxiv_id":"2601.15818","citing_title":"Muon beams towards muonium physics: progress and prospects","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2508.07922","citing_title":"Positron Transport System for Muonium-to-Antimuonium Conversion Experiment","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2511.08679","citing_title":"Hunting for Neutrino Texture Zeros with Muon and Tau Flavor Violation","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"2601.18237","citing_title":"Revisiting $\\mu$-$e$ conversion in $R$-parity violating SUSY","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2604.26817","citing_title":"When Two Loops Matter: Electroweak Precision in the SMEFT","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2604.11889","citing_title":"ALP production in Lepton Flavour Violating meson, tau and gauge boson decays","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08396","citing_title":"Search for the lepton-flavour violating decays $B^+ \\to \\pi^+ \\mu^\\pm e^\\mp$","ref_index":1,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/J5T5DUEFUBWDOJM2CJROFONIPZ","json":"https://pith.science/pith/J5T5DUEFUBWDOJM2CJROFONIPZ.json","graph_json":"https://pith.science/api/pith-number/J5T5DUEFUBWDOJM2CJROFONIPZ/graph.json","events_json":"https://pith.science/api/pith-number/J5T5DUEFUBWDOJM2CJROFONIPZ/events.json","paper":"https://pith.science/paper/J5T5DUEF"},"agent_actions":{"view_html":"https://pith.science/pith/J5T5DUEFUBWDOJM2CJROFONIPZ","download_json":"https://pith.science/pith/J5T5DUEFUBWDOJM2CJROFONIPZ.json","view_paper":"https://pith.science/paper/J5T5DUEF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.00294&json=true","fetch_graph":"https://pith.science/api/pith-number/J5T5DUEFUBWDOJM2CJROFONIPZ/graph.json","fetch_events":"https://pith.science/api/pith-number/J5T5DUEFUBWDOJM2CJROFONIPZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J5T5DUEFUBWDOJM2CJROFONIPZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J5T5DUEFUBWDOJM2CJROFONIPZ/action/storage_attestation","attest_author":"https://pith.science/pith/J5T5DUEFUBWDOJM2CJROFONIPZ/action/author_attestation","sign_citation":"https://pith.science/pith/J5T5DUEFUBWDOJM2CJROFONIPZ/action/citation_signature","submit_replication":"https://pith.science/pith/J5T5DUEFUBWDOJM2CJROFONIPZ/action/replication_record"}},"created_at":"2026-05-18T00:24:35.224669+00:00","updated_at":"2026-05-18T00:24:35.224669+00:00"}