{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:3HLAWDW4KDHSORHY7ASUW42WRM","short_pith_number":"pith:3HLAWDW4","schema_version":"1.0","canonical_sha256":"d9d60b0edc50cf2744f8f8254b73568b257f6f05b91470121073c3038ac9bcca","source":{"kind":"arxiv","id":"1503.08055","version":1},"attestation_state":"computed","paper":{"title":"Measuring BR($h \\to \\tau ^+ \\tau ^-$) at the ILC: a full simulation study","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"Harumichi Yokoyama, Keisuke Fujii, Shin-ichi Kawada, Taikan Suehara, Tohru Takahashi, Tomohiko Tanabe","submitted_at":"2015-03-27T12:54:56Z","abstract_excerpt":"We evaluate the expected measurement accuracy of the branching ratio of the Standard Model Higgs boson decaying into tau pairs at the ILC with a full simulation of the ILD detector concept. We assume a Higgs mass of 125 GeV, a branching ratio of BR($h \\to \\tau ^+ \\tau ^-$) = 6.32%, a beam polarization of electron (positron) of -0.8(+0.3), and an integrated luminosity of 250 fb$^{-1}$. The Higgs-strahlung process $e^+ e^- \\to Zh$ with $Z \\to q\\overline{q}$ is analyzed. We estimate the measurement accuracy of the branching ratio $\\Delta (\\sigma \\times \\mathrm{BR}) / (\\sigma \\times \\mathrm{BR})$ "},"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":"1503.08055","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2015-03-27T12:54:56Z","cross_cats_sorted":[],"title_canon_sha256":"b944d17e3228f34be8bdd374dd45f4c0e68b475e624c14f2c4292557936a8fe8","abstract_canon_sha256":"dd0fb2190f8a82386cda7edf76d986d751b71c519e98890ce9498dd4d2962bbf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:20:11.630362Z","signature_b64":"tr4Zt9CJ6XjSoVo9Vbfy5qqJz6ZzlNSZqC8hDvHcQqDB/RdLxd2WEhds49PzfqcrRrgojED/b3M9zZdsWCCpAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d9d60b0edc50cf2744f8f8254b73568b257f6f05b91470121073c3038ac9bcca","last_reissued_at":"2026-05-18T02:20:11.629866Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:20:11.629866Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measuring BR($h \\to \\tau ^+ \\tau ^-$) at the ILC: a full simulation study","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"Harumichi Yokoyama, Keisuke Fujii, Shin-ichi Kawada, Taikan Suehara, Tohru Takahashi, Tomohiko Tanabe","submitted_at":"2015-03-27T12:54:56Z","abstract_excerpt":"We evaluate the expected measurement accuracy of the branching ratio of the Standard Model Higgs boson decaying into tau pairs at the ILC with a full simulation of the ILD detector concept. We assume a Higgs mass of 125 GeV, a branching ratio of BR($h \\to \\tau ^+ \\tau ^-$) = 6.32%, a beam polarization of electron (positron) of -0.8(+0.3), and an integrated luminosity of 250 fb$^{-1}$. The Higgs-strahlung process $e^+ e^- \\to Zh$ with $Z \\to q\\overline{q}$ is analyzed. We estimate the measurement accuracy of the branching ratio $\\Delta (\\sigma \\times \\mathrm{BR}) / (\\sigma \\times \\mathrm{BR})$ "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.08055","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":"1503.08055","created_at":"2026-05-18T02:20:11.629942+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.08055v1","created_at":"2026-05-18T02:20:11.629942+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.08055","created_at":"2026-05-18T02:20:11.629942+00:00"},{"alias_kind":"pith_short_12","alias_value":"3HLAWDW4KDHS","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_16","alias_value":"3HLAWDW4KDHSORHY","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_8","alias_value":"3HLAWDW4","created_at":"2026-05-18T12:29:02.477457+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3HLAWDW4KDHSORHY7ASUW42WRM","json":"https://pith.science/pith/3HLAWDW4KDHSORHY7ASUW42WRM.json","graph_json":"https://pith.science/api/pith-number/3HLAWDW4KDHSORHY7ASUW42WRM/graph.json","events_json":"https://pith.science/api/pith-number/3HLAWDW4KDHSORHY7ASUW42WRM/events.json","paper":"https://pith.science/paper/3HLAWDW4"},"agent_actions":{"view_html":"https://pith.science/pith/3HLAWDW4KDHSORHY7ASUW42WRM","download_json":"https://pith.science/pith/3HLAWDW4KDHSORHY7ASUW42WRM.json","view_paper":"https://pith.science/paper/3HLAWDW4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.08055&json=true","fetch_graph":"https://pith.science/api/pith-number/3HLAWDW4KDHSORHY7ASUW42WRM/graph.json","fetch_events":"https://pith.science/api/pith-number/3HLAWDW4KDHSORHY7ASUW42WRM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3HLAWDW4KDHSORHY7ASUW42WRM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3HLAWDW4KDHSORHY7ASUW42WRM/action/storage_attestation","attest_author":"https://pith.science/pith/3HLAWDW4KDHSORHY7ASUW42WRM/action/author_attestation","sign_citation":"https://pith.science/pith/3HLAWDW4KDHSORHY7ASUW42WRM/action/citation_signature","submit_replication":"https://pith.science/pith/3HLAWDW4KDHSORHY7ASUW42WRM/action/replication_record"}},"created_at":"2026-05-18T02:20:11.629942+00:00","updated_at":"2026-05-18T02:20:11.629942+00:00"}