{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:L2AQVWYYRPEGVOKRAY4HUPXO2R","short_pith_number":"pith:L2AQVWYY","schema_version":"1.0","canonical_sha256":"5e810adb188bc86ab95106387a3eeed46640eb5e31b4de97c9fc3157b8942c52","source":{"kind":"arxiv","id":"2206.05901","version":2},"attestation_state":"computed","paper":{"title":"Identical particle and lepton mass effects in the decay $H\\to Z^\\ast(\\to\\tau^+\\tau^-)+Z^\\ast(\\to\\tau^+\\tau^-)$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Lauri Kaldam\\\"ae, Maria Naeem, Stefan Groote","submitted_at":"2022-06-13T04:37:52Z","abstract_excerpt":"We consider identical particle and lepton mass effects in the cascade decay $H\\to Z^\\ast(\\to\\tau^+\\tau^-)+Z^\\ast(\\to\\tau^+\\tau^-)$. Since the scale of the problem is set by the off-shellness $p_a^2$ and $p_b^2$ of the respective gauge bosons in the limits ($4m_\\tau^2\\le p_a^2,p_b^2\\le (m_H-2m_\\tau)^2$) and not by $m_H^2$, lepton mass effects are nonnegligible in particular close to the threshold of the off-shell decays. We calculate the rates and single angle decay distributions and compare them with the corresponding rates and single angle decay distributions for the nonidentical particle dec"},"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":"2206.05901","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-06-13T04:37:52Z","cross_cats_sorted":[],"title_canon_sha256":"2288810339c7ded5e2ecb04c0b64593c73ac268ce4d0d157e7447248cc8da95c","abstract_canon_sha256":"1cdeac05ce9ec1c624df0a93400f47a5d51c472ac6f0a96acb35be36903fc443"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:18:16.810632Z","signature_b64":"/XdB8xxaGoIVrcT+aupF65mBGCj3A1l3E5M0WbtlOccxDQEun40xOUEEkGUICWrCoAOEQ9T9pABzLoqnyGkQCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e810adb188bc86ab95106387a3eeed46640eb5e31b4de97c9fc3157b8942c52","last_reissued_at":"2026-07-05T06:18:16.810191Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:18:16.810191Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Identical particle and lepton mass effects in the decay $H\\to Z^\\ast(\\to\\tau^+\\tau^-)+Z^\\ast(\\to\\tau^+\\tau^-)$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Lauri Kaldam\\\"ae, Maria Naeem, Stefan Groote","submitted_at":"2022-06-13T04:37:52Z","abstract_excerpt":"We consider identical particle and lepton mass effects in the cascade decay $H\\to Z^\\ast(\\to\\tau^+\\tau^-)+Z^\\ast(\\to\\tau^+\\tau^-)$. Since the scale of the problem is set by the off-shellness $p_a^2$ and $p_b^2$ of the respective gauge bosons in the limits ($4m_\\tau^2\\le p_a^2,p_b^2\\le (m_H-2m_\\tau)^2$) and not by $m_H^2$, lepton mass effects are nonnegligible in particular close to the threshold of the off-shell decays. We calculate the rates and single angle decay distributions and compare them with the corresponding rates and single angle decay distributions for the nonidentical particle dec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.05901","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/2206.05901/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":"2206.05901","created_at":"2026-07-05T06:18:16.810251+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.05901v2","created_at":"2026-07-05T06:18:16.810251+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.05901","created_at":"2026-07-05T06:18:16.810251+00:00"},{"alias_kind":"pith_short_12","alias_value":"L2AQVWYYRPEG","created_at":"2026-07-05T06:18:16.810251+00:00"},{"alias_kind":"pith_short_16","alias_value":"L2AQVWYYRPEGVOKR","created_at":"2026-07-05T06:18:16.810251+00:00"},{"alias_kind":"pith_short_8","alias_value":"L2AQVWYY","created_at":"2026-07-05T06:18:16.810251+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.05061","citing_title":"Angular and invariant-mass observables in the four-body Higgs decay $h\\to\\ell\\bar{\\nu}_\\ell\\bar{\\ell}^\\prime\\nu_{\\ell^\\prime}$","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/L2AQVWYYRPEGVOKRAY4HUPXO2R","json":"https://pith.science/pith/L2AQVWYYRPEGVOKRAY4HUPXO2R.json","graph_json":"https://pith.science/api/pith-number/L2AQVWYYRPEGVOKRAY4HUPXO2R/graph.json","events_json":"https://pith.science/api/pith-number/L2AQVWYYRPEGVOKRAY4HUPXO2R/events.json","paper":"https://pith.science/paper/L2AQVWYY"},"agent_actions":{"view_html":"https://pith.science/pith/L2AQVWYYRPEGVOKRAY4HUPXO2R","download_json":"https://pith.science/pith/L2AQVWYYRPEGVOKRAY4HUPXO2R.json","view_paper":"https://pith.science/paper/L2AQVWYY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.05901&json=true","fetch_graph":"https://pith.science/api/pith-number/L2AQVWYYRPEGVOKRAY4HUPXO2R/graph.json","fetch_events":"https://pith.science/api/pith-number/L2AQVWYYRPEGVOKRAY4HUPXO2R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L2AQVWYYRPEGVOKRAY4HUPXO2R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L2AQVWYYRPEGVOKRAY4HUPXO2R/action/storage_attestation","attest_author":"https://pith.science/pith/L2AQVWYYRPEGVOKRAY4HUPXO2R/action/author_attestation","sign_citation":"https://pith.science/pith/L2AQVWYYRPEGVOKRAY4HUPXO2R/action/citation_signature","submit_replication":"https://pith.science/pith/L2AQVWYYRPEGVOKRAY4HUPXO2R/action/replication_record"}},"created_at":"2026-07-05T06:18:16.810251+00:00","updated_at":"2026-07-05T06:18:16.810251+00:00"}