{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:4BWTELAPNHDJESG4LLAIRXD4BE","short_pith_number":"pith:4BWTELAP","schema_version":"1.0","canonical_sha256":"e06d322c0f69c69248dc5ac088dc7c092871fa45bbc54f90c8512f975405de1a","source":{"kind":"arxiv","id":"1905.03296","version":2},"attestation_state":"computed","paper":{"title":"Higgs interference effects at the one-loop level in the 1-Higgs-Singlet extension of the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alexander Lind, Nikolas Kauer, Philipp Maierh\\\"ofer, WeiMin Song","submitted_at":"2019-05-08T18:58:11Z","abstract_excerpt":"A detailed study of Higgs interference effects at the one-loop level in the 1-Higgs-Singlet extension of the Standard Model (1HSM) is presented for the WW and tt decay modes with fully leptonic WW decay. We explore interference effects for benchmark points with a heavy Higgs mass that significantly exceeds 2*m_t. In the WW channel, the Higgs signal and the interfering continuum background are loop induced. In the tt channel, which features a tree-level background, we also calculate the interference with the one-loop background, which, due to the appearance of the absorptive part, is found to d"},"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":"1905.03296","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-05-08T18:58:11Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"15c743000041aad4ed9676ad5acc4531b2912141e1e70c9c77810f3a9e78d06e","abstract_canon_sha256":"cb59ff33c4ce5063d9ce6203bd3707f9827dfd3ec3b72cbb891a14aa5dd27c54"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:40:10.802072Z","signature_b64":"+newYgBg1mpOvbly0GGsgrMuvaIpE6lyJRtyDVXVuDW/pGmBmHZfpZdA9b+UczUE9CpN05xDlQWu7DNwo2BrDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e06d322c0f69c69248dc5ac088dc7c092871fa45bbc54f90c8512f975405de1a","last_reissued_at":"2026-05-17T23:40:10.801535Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:40:10.801535Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs interference effects at the one-loop level in the 1-Higgs-Singlet extension of the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alexander Lind, Nikolas Kauer, Philipp Maierh\\\"ofer, WeiMin Song","submitted_at":"2019-05-08T18:58:11Z","abstract_excerpt":"A detailed study of Higgs interference effects at the one-loop level in the 1-Higgs-Singlet extension of the Standard Model (1HSM) is presented for the WW and tt decay modes with fully leptonic WW decay. We explore interference effects for benchmark points with a heavy Higgs mass that significantly exceeds 2*m_t. In the WW channel, the Higgs signal and the interfering continuum background are loop induced. In the tt channel, which features a tree-level background, we also calculate the interference with the one-loop background, which, due to the appearance of the absorptive part, is found to d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.03296","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":"1905.03296","created_at":"2026-05-17T23:40:10.801630+00:00"},{"alias_kind":"arxiv_version","alias_value":"1905.03296v2","created_at":"2026-05-17T23:40:10.801630+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.03296","created_at":"2026-05-17T23:40:10.801630+00:00"},{"alias_kind":"pith_short_12","alias_value":"4BWTELAPNHDJ","created_at":"2026-05-18T12:33:10.108867+00:00"},{"alias_kind":"pith_short_16","alias_value":"4BWTELAPNHDJESG4","created_at":"2026-05-18T12:33:10.108867+00:00"},{"alias_kind":"pith_short_8","alias_value":"4BWTELAP","created_at":"2026-05-18T12:33:10.108867+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/4BWTELAPNHDJESG4LLAIRXD4BE","json":"https://pith.science/pith/4BWTELAPNHDJESG4LLAIRXD4BE.json","graph_json":"https://pith.science/api/pith-number/4BWTELAPNHDJESG4LLAIRXD4BE/graph.json","events_json":"https://pith.science/api/pith-number/4BWTELAPNHDJESG4LLAIRXD4BE/events.json","paper":"https://pith.science/paper/4BWTELAP"},"agent_actions":{"view_html":"https://pith.science/pith/4BWTELAPNHDJESG4LLAIRXD4BE","download_json":"https://pith.science/pith/4BWTELAPNHDJESG4LLAIRXD4BE.json","view_paper":"https://pith.science/paper/4BWTELAP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1905.03296&json=true","fetch_graph":"https://pith.science/api/pith-number/4BWTELAPNHDJESG4LLAIRXD4BE/graph.json","fetch_events":"https://pith.science/api/pith-number/4BWTELAPNHDJESG4LLAIRXD4BE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4BWTELAPNHDJESG4LLAIRXD4BE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4BWTELAPNHDJESG4LLAIRXD4BE/action/storage_attestation","attest_author":"https://pith.science/pith/4BWTELAPNHDJESG4LLAIRXD4BE/action/author_attestation","sign_citation":"https://pith.science/pith/4BWTELAPNHDJESG4LLAIRXD4BE/action/citation_signature","submit_replication":"https://pith.science/pith/4BWTELAPNHDJESG4LLAIRXD4BE/action/replication_record"}},"created_at":"2026-05-17T23:40:10.801630+00:00","updated_at":"2026-05-17T23:40:10.801630+00:00"}