{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:Y564IBP3ILGGBUR3DFO6GIAYMC","short_pith_number":"pith:Y564IBP3","schema_version":"1.0","canonical_sha256":"c77dc405fb42cc60d23b195de3201860a813ab8f488b20e36961484d7b39d343","source":{"kind":"arxiv","id":"1503.07394","version":2},"attestation_state":"computed","paper":{"title":"Higgs boson decay into four leptons at NLOPS electroweak accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Carlo M. Carloni Calame, Fulvio Piccinini, Guido Montagna, Oreste Nicrosini, Stefano Boselli","submitted_at":"2015-03-25T14:33:50Z","abstract_excerpt":"In view of precision studies of the Higgs sector at the Run II of the LHC, the improvement of the accuracy of the theoretical prediction is becoming a pressing issue. In this framework, we detail a calculation of the full Next-to-Leading Order (NLO) electroweak corrections to Higgs boson decay into four charged leptons, by considering the gold-plated channel H -> Z(*) Z(*) -> 2l 2l', l,l' = e, mu. We match the NLO corrections with a QED Parton Shower (PS), in order to simulate exclusive multiple photon emission and provide novel results at NLOPS electroweak accuracy. We compare our NLO predict"},"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":"1503.07394","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-03-25T14:33:50Z","cross_cats_sorted":[],"title_canon_sha256":"f89fa96618dc0688d5eaf4e9330b0a8184eae7e3bfaca91d97b34d8c747aa843","abstract_canon_sha256":"240b9c440f83e75267d30616378ed9708b4b55b56fc59c5e723e6ad4bbd8ea55"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:57.585585Z","signature_b64":"7T33U+wYzqAM6Tx0pOzlm6gdvt+Pe63OGeGcde4FqUaqgQdsPVhL4zXkoEyIjeKVRxcq6EwBYY6RBb2qjsZeBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c77dc405fb42cc60d23b195de3201860a813ab8f488b20e36961484d7b39d343","last_reissued_at":"2026-05-18T01:59:57.585109Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:57.585109Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs boson decay into four leptons at NLOPS electroweak accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Carlo M. Carloni Calame, Fulvio Piccinini, Guido Montagna, Oreste Nicrosini, Stefano Boselli","submitted_at":"2015-03-25T14:33:50Z","abstract_excerpt":"In view of precision studies of the Higgs sector at the Run II of the LHC, the improvement of the accuracy of the theoretical prediction is becoming a pressing issue. In this framework, we detail a calculation of the full Next-to-Leading Order (NLO) electroweak corrections to Higgs boson decay into four charged leptons, by considering the gold-plated channel H -> Z(*) Z(*) -> 2l 2l', l,l' = e, mu. We match the NLO corrections with a QED Parton Shower (PS), in order to simulate exclusive multiple photon emission and provide novel results at NLOPS electroweak accuracy. We compare our NLO predict"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.07394","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":"1503.07394","created_at":"2026-05-18T01:59:57.585184+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.07394v2","created_at":"2026-05-18T01:59:57.585184+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.07394","created_at":"2026-05-18T01:59:57.585184+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y564IBP3ILGG","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y564IBP3ILGGBUR3","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y564IBP3","created_at":"2026-05-18T12:29:50.041715+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2404.06335","citing_title":"Software and computing for Run 3 of the ATLAS experiment at the LHC","ref_index":129,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Y564IBP3ILGGBUR3DFO6GIAYMC","json":"https://pith.science/pith/Y564IBP3ILGGBUR3DFO6GIAYMC.json","graph_json":"https://pith.science/api/pith-number/Y564IBP3ILGGBUR3DFO6GIAYMC/graph.json","events_json":"https://pith.science/api/pith-number/Y564IBP3ILGGBUR3DFO6GIAYMC/events.json","paper":"https://pith.science/paper/Y564IBP3"},"agent_actions":{"view_html":"https://pith.science/pith/Y564IBP3ILGGBUR3DFO6GIAYMC","download_json":"https://pith.science/pith/Y564IBP3ILGGBUR3DFO6GIAYMC.json","view_paper":"https://pith.science/paper/Y564IBP3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.07394&json=true","fetch_graph":"https://pith.science/api/pith-number/Y564IBP3ILGGBUR3DFO6GIAYMC/graph.json","fetch_events":"https://pith.science/api/pith-number/Y564IBP3ILGGBUR3DFO6GIAYMC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y564IBP3ILGGBUR3DFO6GIAYMC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y564IBP3ILGGBUR3DFO6GIAYMC/action/storage_attestation","attest_author":"https://pith.science/pith/Y564IBP3ILGGBUR3DFO6GIAYMC/action/author_attestation","sign_citation":"https://pith.science/pith/Y564IBP3ILGGBUR3DFO6GIAYMC/action/citation_signature","submit_replication":"https://pith.science/pith/Y564IBP3ILGGBUR3DFO6GIAYMC/action/replication_record"}},"created_at":"2026-05-18T01:59:57.585184+00:00","updated_at":"2026-05-18T01:59:57.585184+00:00"}