{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:QRECM5VVKZ5U46DUHI73SNN7DI","short_pith_number":"pith:QRECM5VV","schema_version":"1.0","canonical_sha256":"84482676b5567b4e78743a3fb935bf1a07d4e6d521b300d71ed5ede6f4e4be63","source":{"kind":"arxiv","id":"1912.10477","version":1},"attestation_state":"computed","paper":{"title":"Electroweak Phase Transition in Non-Minimal Higgs Sectors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. M\\\"uller, M. M\\\"uhlleitner, P. Basler","submitted_at":"2019-12-22T17:01:00Z","abstract_excerpt":"Higgs sector extensions beyond the Standard Model (BSM) provide additional sources of CP violation and further scalar states that help to trigger a strong first order electroweak phase transition (SFOEWPT) required to generate the observed baryon asymmetry of the Universe through electroweak baryogenesis. We investigate the CP-violating 2-Higgs-Doublet Model (C2HDM) and the Next-to-Minimal 2-Higgs-Doublet Model (N2HDM) with respect to their potential to generate an SFOEWPT while being compatible with all relevant and recent theoretical and experimental constraints. The implications of an SFOEW"},"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":"1912.10477","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-12-22T17:01:00Z","cross_cats_sorted":[],"title_canon_sha256":"339c556a1019224f9b3dc194b7eefb8ea5f6d3f958a49760933da2a47a30b87d","abstract_canon_sha256":"e576f3cab50607bf86e8165744cefd07cd8301ce9378369d77031eb83dc9aad2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:04:10.570736Z","signature_b64":"Nhp/KKdXxLnn7oqVnO3Ijggnnm6rt6wBKcdKI08/XuAyZPhDh1P+ON53npNgDp3YCsVdsc+sEwbTNiV8YmTXBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"84482676b5567b4e78743a3fb935bf1a07d4e6d521b300d71ed5ede6f4e4be63","last_reissued_at":"2026-07-05T01:04:10.570275Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:04:10.570275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electroweak Phase Transition in Non-Minimal Higgs Sectors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. M\\\"uller, M. M\\\"uhlleitner, P. Basler","submitted_at":"2019-12-22T17:01:00Z","abstract_excerpt":"Higgs sector extensions beyond the Standard Model (BSM) provide additional sources of CP violation and further scalar states that help to trigger a strong first order electroweak phase transition (SFOEWPT) required to generate the observed baryon asymmetry of the Universe through electroweak baryogenesis. We investigate the CP-violating 2-Higgs-Doublet Model (C2HDM) and the Next-to-Minimal 2-Higgs-Doublet Model (N2HDM) with respect to their potential to generate an SFOEWPT while being compatible with all relevant and recent theoretical and experimental constraints. The implications of an SFOEW"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1912.10477","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1912.10477/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":"1912.10477","created_at":"2026-07-05T01:04:10.570340+00:00"},{"alias_kind":"arxiv_version","alias_value":"1912.10477v1","created_at":"2026-07-05T01:04:10.570340+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1912.10477","created_at":"2026-07-05T01:04:10.570340+00:00"},{"alias_kind":"pith_short_12","alias_value":"QRECM5VVKZ5U","created_at":"2026-07-05T01:04:10.570340+00:00"},{"alias_kind":"pith_short_16","alias_value":"QRECM5VVKZ5U46DU","created_at":"2026-07-05T01:04:10.570340+00:00"},{"alias_kind":"pith_short_8","alias_value":"QRECM5VV","created_at":"2026-07-05T01:04:10.570340+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.19425","citing_title":"LeWRON: Agentic Analysis of Electroweak Phase Transitions","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2512.17002","citing_title":"Intrinsic Properties of Large CP Violation in the Complex Two-Higgs-Doublet Model","ref_index":18,"is_internal_anchor":false},{"citing_arxiv_id":"2509.01682","citing_title":"Towards a Unified Framework for Pseudo-Nambu-Goldstone Dark Matter and Electroweak Baryogenesis","ref_index":65,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QRECM5VVKZ5U46DUHI73SNN7DI","json":"https://pith.science/pith/QRECM5VVKZ5U46DUHI73SNN7DI.json","graph_json":"https://pith.science/api/pith-number/QRECM5VVKZ5U46DUHI73SNN7DI/graph.json","events_json":"https://pith.science/api/pith-number/QRECM5VVKZ5U46DUHI73SNN7DI/events.json","paper":"https://pith.science/paper/QRECM5VV"},"agent_actions":{"view_html":"https://pith.science/pith/QRECM5VVKZ5U46DUHI73SNN7DI","download_json":"https://pith.science/pith/QRECM5VVKZ5U46DUHI73SNN7DI.json","view_paper":"https://pith.science/paper/QRECM5VV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1912.10477&json=true","fetch_graph":"https://pith.science/api/pith-number/QRECM5VVKZ5U46DUHI73SNN7DI/graph.json","fetch_events":"https://pith.science/api/pith-number/QRECM5VVKZ5U46DUHI73SNN7DI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QRECM5VVKZ5U46DUHI73SNN7DI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QRECM5VVKZ5U46DUHI73SNN7DI/action/storage_attestation","attest_author":"https://pith.science/pith/QRECM5VVKZ5U46DUHI73SNN7DI/action/author_attestation","sign_citation":"https://pith.science/pith/QRECM5VVKZ5U46DUHI73SNN7DI/action/citation_signature","submit_replication":"https://pith.science/pith/QRECM5VVKZ5U46DUHI73SNN7DI/action/replication_record"}},"created_at":"2026-07-05T01:04:10.570340+00:00","updated_at":"2026-07-05T01:04:10.570340+00:00"}