{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:W47RYBYHKBFRNIX2SQSU2R4FY4","short_pith_number":"pith:W47RYBYH","schema_version":"1.0","canonical_sha256":"b73f1c0707504b16a2fa94254d4785c70ba2c1501345d005799bdc31b2c7e235","source":{"kind":"arxiv","id":"hep-ex/0506072","version":1},"attestation_state":"computed","paper":{"title":"Branching ratios and spectral functions of tau decays: final ALEPH measurements and physics implications","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"the ALEPH Collaboration","submitted_at":"2005-06-28T19:41:25Z","abstract_excerpt":"The full LEP-1 data set collected with the ALEPH detector at the $Z$ pole during 1991-1995 is analysed in order to measure the $\\tau$ decay branching fractions. Extensive systematic studies are performed, in order to match the large statistics of the data sample corresponding to over 300 000 measured and identified $\\tau$ decays. Branching fractions are obtained for the two leptonic channels and eleven hadronic channels defined by their respective numbers of charged particles and $\\pi^0$'s. Using previously published ALEPH results on final states with charged and neutral kaons, corrections are"},"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-ex/0506072","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2005-06-28T19:41:25Z","cross_cats_sorted":[],"title_canon_sha256":"0879d3f12a3a9d8198e44a0ca30708d93e4b5dff061260616706e1cd0236c812","abstract_canon_sha256":"09bdf63c91f3a038738b9b3bfa01e9111fca7cbd2f399523e640d656f0ec0720"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:30.469241Z","signature_b64":"EcqJKxDHh++oolDb2zFWZXdMW23Fw/ovNDb2GaCkFPX2nbwgGW5Gj5GMAqGLWLaZspbEefOh+BnGfhTCmW7qCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b73f1c0707504b16a2fa94254d4785c70ba2c1501345d005799bdc31b2c7e235","last_reissued_at":"2026-05-18T03:47:30.468809Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:30.468809Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Branching ratios and spectral functions of tau decays: final ALEPH measurements and physics implications","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"the ALEPH Collaboration","submitted_at":"2005-06-28T19:41:25Z","abstract_excerpt":"The full LEP-1 data set collected with the ALEPH detector at the $Z$ pole during 1991-1995 is analysed in order to measure the $\\tau$ decay branching fractions. Extensive systematic studies are performed, in order to match the large statistics of the data sample corresponding to over 300 000 measured and identified $\\tau$ decays. Branching fractions are obtained for the two leptonic channels and eleven hadronic channels defined by their respective numbers of charged particles and $\\pi^0$'s. Using previously published ALEPH results on final states with charged and neutral kaons, corrections are"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0506072","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":"hep-ex/0506072","created_at":"2026-05-18T03:47:30.468868+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0506072v1","created_at":"2026-05-18T03:47:30.468868+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0506072","created_at":"2026-05-18T03:47:30.468868+00:00"},{"alias_kind":"pith_short_12","alias_value":"W47RYBYHKBFR","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_16","alias_value":"W47RYBYHKBFRNIX2","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_8","alias_value":"W47RYBYH","created_at":"2026-05-18T12:25:53.939244+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2006.04822","citing_title":"The anomalous magnetic moment of the muon in the Standard Model","ref_index":180,"is_internal_anchor":true},{"citing_arxiv_id":"2512.18382","citing_title":"Lepton anomalous magnetic moments: Theory","ref_index":97,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11277","citing_title":"Hadronic tau decays at higher orders in QCD","ref_index":102,"is_internal_anchor":true},{"citing_arxiv_id":"2505.21476","citing_title":"The anomalous magnetic moment of the muon in the Standard Model: an update","ref_index":188,"is_internal_anchor":true},{"citing_arxiv_id":"2605.12205","citing_title":"Comparison of the hadronic vacuum polarization between hadronic $\\tau$-decay data and lattice QCD","ref_index":24,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W47RYBYHKBFRNIX2SQSU2R4FY4","json":"https://pith.science/pith/W47RYBYHKBFRNIX2SQSU2R4FY4.json","graph_json":"https://pith.science/api/pith-number/W47RYBYHKBFRNIX2SQSU2R4FY4/graph.json","events_json":"https://pith.science/api/pith-number/W47RYBYHKBFRNIX2SQSU2R4FY4/events.json","paper":"https://pith.science/paper/W47RYBYH"},"agent_actions":{"view_html":"https://pith.science/pith/W47RYBYHKBFRNIX2SQSU2R4FY4","download_json":"https://pith.science/pith/W47RYBYHKBFRNIX2SQSU2R4FY4.json","view_paper":"https://pith.science/paper/W47RYBYH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0506072&json=true","fetch_graph":"https://pith.science/api/pith-number/W47RYBYHKBFRNIX2SQSU2R4FY4/graph.json","fetch_events":"https://pith.science/api/pith-number/W47RYBYHKBFRNIX2SQSU2R4FY4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W47RYBYHKBFRNIX2SQSU2R4FY4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W47RYBYHKBFRNIX2SQSU2R4FY4/action/storage_attestation","attest_author":"https://pith.science/pith/W47RYBYHKBFRNIX2SQSU2R4FY4/action/author_attestation","sign_citation":"https://pith.science/pith/W47RYBYHKBFRNIX2SQSU2R4FY4/action/citation_signature","submit_replication":"https://pith.science/pith/W47RYBYHKBFRNIX2SQSU2R4FY4/action/replication_record"}},"created_at":"2026-05-18T03:47:30.468868+00:00","updated_at":"2026-05-18T03:47:30.468868+00:00"}