{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:PPCNLHHKZR5LX7YKEO4YW3QL2G","short_pith_number":"pith:PPCNLHHK","schema_version":"1.0","canonical_sha256":"7bc4d59ceacc7abbff0a23b98b6e0bd1a054839cfb5b155949044c849b1ed630","source":{"kind":"arxiv","id":"hep-ph/0206056","version":2},"attestation_state":"computed","paper":{"title":"\\tau - \\mu Flavor Violation as a Probe of the Scale of New Physics","license":"","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"hep-ph","authors_text":"Deirdre Black, Hong-Jian He, Marc Sher, Tao Han","submitted_at":"2002-06-05T19:53:28Z","abstract_excerpt":"Motivated by the recent strong experimental evidence of large \\nu_mu-\\nu_tau neutrino mixing, we explore current bounds on the analogous mixing in the charged lepton sector. We present a general formalism for dimension-6 fermionic effective operators involving tau-mu mixing with typical Lorentz structure (\\bar{mu} \\Gamma tau)(\\bar{q}^a \\Gamma {q}^b), and discuss their relationship to the standard model gauge symmetry and the underlying flavor dynamics. We derive the low-energy constraints on the new physics scale associated with each operator, mostly from current experimental bounds on rare de"},"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/0206056","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-06-05T19:53:28Z","cross_cats_sorted":["hep-ex","nucl-ex"],"title_canon_sha256":"818496150fb409ab888464c515971f9e2a550acf850de8cff0d23f974e9e7cf0","abstract_canon_sha256":"e687f596cc7ff72477684712c62850cbfee8bf79627c11b1fc3b3ac3cbdadeec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:26:42.125763Z","signature_b64":"Ov9PFgtWo1ElmbScEgUAZmmpHjtsJNvl2uBwhXD7W+GO9uzErYDAavOgzyy4/1ZRpexNicNVhf5lunrDv0ZcAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7bc4d59ceacc7abbff0a23b98b6e0bd1a054839cfb5b155949044c849b1ed630","last_reissued_at":"2026-07-04T15:26:42.125369Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:26:42.125369Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"\\tau - \\mu Flavor Violation as a Probe of the Scale of New Physics","license":"","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"hep-ph","authors_text":"Deirdre Black, Hong-Jian He, Marc Sher, Tao Han","submitted_at":"2002-06-05T19:53:28Z","abstract_excerpt":"Motivated by the recent strong experimental evidence of large \\nu_mu-\\nu_tau neutrino mixing, we explore current bounds on the analogous mixing in the charged lepton sector. We present a general formalism for dimension-6 fermionic effective operators involving tau-mu mixing with typical Lorentz structure (\\bar{mu} \\Gamma tau)(\\bar{q}^a \\Gamma {q}^b), and discuss their relationship to the standard model gauge symmetry and the underlying flavor dynamics. We derive the low-energy constraints on the new physics scale associated with each operator, mostly from current experimental bounds on rare de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0206056","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/0206056/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/0206056","created_at":"2026-07-04T15:26:42.125429+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0206056v2","created_at":"2026-07-04T15:26:42.125429+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0206056","created_at":"2026-07-04T15:26:42.125429+00:00"},{"alias_kind":"pith_short_12","alias_value":"PPCNLHHKZR5L","created_at":"2026-07-04T15:26:42.125429+00:00"},{"alias_kind":"pith_short_16","alias_value":"PPCNLHHKZR5LX7YK","created_at":"2026-07-04T15:26:42.125429+00:00"},{"alias_kind":"pith_short_8","alias_value":"PPCNLHHK","created_at":"2026-07-04T15:26:42.125429+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.19723","citing_title":"Charged Lepton Flavor Violation at Neutrino Telescopes","ref_index":43,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PPCNLHHKZR5LX7YKEO4YW3QL2G","json":"https://pith.science/pith/PPCNLHHKZR5LX7YKEO4YW3QL2G.json","graph_json":"https://pith.science/api/pith-number/PPCNLHHKZR5LX7YKEO4YW3QL2G/graph.json","events_json":"https://pith.science/api/pith-number/PPCNLHHKZR5LX7YKEO4YW3QL2G/events.json","paper":"https://pith.science/paper/PPCNLHHK"},"agent_actions":{"view_html":"https://pith.science/pith/PPCNLHHKZR5LX7YKEO4YW3QL2G","download_json":"https://pith.science/pith/PPCNLHHKZR5LX7YKEO4YW3QL2G.json","view_paper":"https://pith.science/paper/PPCNLHHK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0206056&json=true","fetch_graph":"https://pith.science/api/pith-number/PPCNLHHKZR5LX7YKEO4YW3QL2G/graph.json","fetch_events":"https://pith.science/api/pith-number/PPCNLHHKZR5LX7YKEO4YW3QL2G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PPCNLHHKZR5LX7YKEO4YW3QL2G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PPCNLHHKZR5LX7YKEO4YW3QL2G/action/storage_attestation","attest_author":"https://pith.science/pith/PPCNLHHKZR5LX7YKEO4YW3QL2G/action/author_attestation","sign_citation":"https://pith.science/pith/PPCNLHHKZR5LX7YKEO4YW3QL2G/action/citation_signature","submit_replication":"https://pith.science/pith/PPCNLHHKZR5LX7YKEO4YW3QL2G/action/replication_record"}},"created_at":"2026-07-04T15:26:42.125429+00:00","updated_at":"2026-07-04T15:26:42.125429+00:00"}