{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:ILELIBWG4EAHKN76UVPSZY625F","short_pith_number":"pith:ILELIBWG","schema_version":"1.0","canonical_sha256":"42c8b406c6e1007537fea55f2ce3dae9553e25fcfc71253ada81fdfc8daa37f6","source":{"kind":"arxiv","id":"1407.5342","version":2},"attestation_state":"computed","paper":{"title":"Singlet-Catalyzed Electroweak Phase Transitions and Precision Higgs Studies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Carroll L. Wainwright, Michael J. Ramsey-Musolf, Peter Winslow, Stefano Profumo","submitted_at":"2014-07-20T21:55:23Z","abstract_excerpt":"We update the phenomenology of gauge singlet extensions of the Standard Model scalar sector and their implications for the electroweak phase transition. Considering the introduction of one real scalar singlet to the scalar potential, we analyze present constraints on the potential parameters from Higgs coupling measurements at the Large Hadron Collider (LHC) and electroweak precision observables for the kinematic regime in which no new scalar decay modes arise. We then show how future precision measurements of Higgs boson signal strengths and Higgs self-coupling could probe the scalar potentia"},"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":"1407.5342","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-20T21:55:23Z","cross_cats_sorted":[],"title_canon_sha256":"2f190fa433e7f20d1cdb6d99e91171aa62f48b097040eea8ebff442c6cd37d0b","abstract_canon_sha256":"d5e7d9bee1f352498633a5904de3a3627d22b61acee8b327eab16b1937037804"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:25:47.092995Z","signature_b64":"StpKDn9TJSWNud2EpuZ0aQDmvKjRpxjjqmDJMrl+/Q6YOy4bplxkI09dc5SYXgGX5xki0nKBKMLHIbhWlqqdBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"42c8b406c6e1007537fea55f2ce3dae9553e25fcfc71253ada81fdfc8daa37f6","last_reissued_at":"2026-05-18T02:25:47.092348Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:25:47.092348Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Singlet-Catalyzed Electroweak Phase Transitions and Precision Higgs Studies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Carroll L. Wainwright, Michael J. Ramsey-Musolf, Peter Winslow, Stefano Profumo","submitted_at":"2014-07-20T21:55:23Z","abstract_excerpt":"We update the phenomenology of gauge singlet extensions of the Standard Model scalar sector and their implications for the electroweak phase transition. Considering the introduction of one real scalar singlet to the scalar potential, we analyze present constraints on the potential parameters from Higgs coupling measurements at the Large Hadron Collider (LHC) and electroweak precision observables for the kinematic regime in which no new scalar decay modes arise. We then show how future precision measurements of Higgs boson signal strengths and Higgs self-coupling could probe the scalar potentia"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.5342","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":"1407.5342","created_at":"2026-05-18T02:25:47.092452+00:00"},{"alias_kind":"arxiv_version","alias_value":"1407.5342v2","created_at":"2026-05-18T02:25:47.092452+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.5342","created_at":"2026-05-18T02:25:47.092452+00:00"},{"alias_kind":"pith_short_12","alias_value":"ILELIBWG4EAH","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_16","alias_value":"ILELIBWG4EAHKN76","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_8","alias_value":"ILELIBWG","created_at":"2026-05-18T12:28:33.132498+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"1910.13125","citing_title":"Detecting gravitational waves from cosmological phase transitions with LISA: an update","ref_index":76,"is_internal_anchor":true},{"citing_arxiv_id":"2511.00996","citing_title":"Measuring gravitational wave spectrum from electroweak phase transition and Higgs self-couplings","ref_index":54,"is_internal_anchor":true},{"citing_arxiv_id":"2603.18583","citing_title":"Electroweak phase transitions in a $U(1)_D$ extension of the standard model with dimension-six operators: Gravitational waves and LHC signatures","ref_index":18,"is_internal_anchor":true},{"citing_arxiv_id":"2604.27471","citing_title":"Constraints on a Light Singlet Scalar from Combined Exotic Higgs Decays","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00095","citing_title":"A Model of Annihilogenesis","ref_index":7,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ILELIBWG4EAHKN76UVPSZY625F","json":"https://pith.science/pith/ILELIBWG4EAHKN76UVPSZY625F.json","graph_json":"https://pith.science/api/pith-number/ILELIBWG4EAHKN76UVPSZY625F/graph.json","events_json":"https://pith.science/api/pith-number/ILELIBWG4EAHKN76UVPSZY625F/events.json","paper":"https://pith.science/paper/ILELIBWG"},"agent_actions":{"view_html":"https://pith.science/pith/ILELIBWG4EAHKN76UVPSZY625F","download_json":"https://pith.science/pith/ILELIBWG4EAHKN76UVPSZY625F.json","view_paper":"https://pith.science/paper/ILELIBWG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1407.5342&json=true","fetch_graph":"https://pith.science/api/pith-number/ILELIBWG4EAHKN76UVPSZY625F/graph.json","fetch_events":"https://pith.science/api/pith-number/ILELIBWG4EAHKN76UVPSZY625F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ILELIBWG4EAHKN76UVPSZY625F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ILELIBWG4EAHKN76UVPSZY625F/action/storage_attestation","attest_author":"https://pith.science/pith/ILELIBWG4EAHKN76UVPSZY625F/action/author_attestation","sign_citation":"https://pith.science/pith/ILELIBWG4EAHKN76UVPSZY625F/action/citation_signature","submit_replication":"https://pith.science/pith/ILELIBWG4EAHKN76UVPSZY625F/action/replication_record"}},"created_at":"2026-05-18T02:25:47.092452+00:00","updated_at":"2026-05-18T02:25:47.092452+00:00"}