{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:ELFYEDBW4SWTNMLFNEFPGSW6QE","short_pith_number":"pith:ELFYEDBW","schema_version":"1.0","canonical_sha256":"22cb820c36e4ad36b165690af34ade8129e59e843718eba8bea3e54072da706b","source":{"kind":"arxiv","id":"2507.14288","version":1},"attestation_state":"computed","paper":{"title":"The electroweak precision constraints of the 2HDM+S","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cheng Li, Juxiang Li, Shufang Su, Wei Su","submitted_at":"2025-07-18T18:00:18Z","abstract_excerpt":"The 2HDM+S is the singlet extension of the Two-Higgs-Doublets Model (2HDM). The singlet field and its mixing with the 2HDM Higgs sector lead to new contributions to the electroweak precision observables, in particular, the oblique parameters. In this paper, we identify five benchmark cases, where at most one mixing angle is nonzero and analyze the 95% C.L. allowed parameter space by the oblique parameters. In the alignment limit of the 2HDM, we find that other than the usual mass relations of $m_H\\sim m_{H^\\pm}$ or $m_A\\sim m_{H^\\pm}$, electroweak precision measurements also impose an upper li"},"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":"2507.14288","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-07-18T18:00:18Z","cross_cats_sorted":[],"title_canon_sha256":"27a3c512e7c4ae62813fe446cd075db12d01daf18c2a70a5d37c1b1127aa7b9a","abstract_canon_sha256":"818df8e062fffa8d63b137932a594290a6b82f170f3da792913f473b6cd5e71a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:40:03.739569Z","signature_b64":"E0L6Y5tgkHsw4YuxV2SLjmFuAyZ4wtH7q0nfkLjQrJ0yY+5Xo4lJxiAOM5IEq4iVhh77uPcBA1F+p5JzV5QBCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"22cb820c36e4ad36b165690af34ade8129e59e843718eba8bea3e54072da706b","last_reissued_at":"2026-07-05T11:40:03.738966Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:40:03.738966Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The electroweak precision constraints of the 2HDM+S","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cheng Li, Juxiang Li, Shufang Su, Wei Su","submitted_at":"2025-07-18T18:00:18Z","abstract_excerpt":"The 2HDM+S is the singlet extension of the Two-Higgs-Doublets Model (2HDM). The singlet field and its mixing with the 2HDM Higgs sector lead to new contributions to the electroweak precision observables, in particular, the oblique parameters. In this paper, we identify five benchmark cases, where at most one mixing angle is nonzero and analyze the 95% C.L. allowed parameter space by the oblique parameters. In the alignment limit of the 2HDM, we find that other than the usual mass relations of $m_H\\sim m_{H^\\pm}$ or $m_A\\sim m_{H^\\pm}$, electroweak precision measurements also impose an upper li"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.14288","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/2507.14288/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":"2507.14288","created_at":"2026-07-05T11:40:03.739037+00:00"},{"alias_kind":"arxiv_version","alias_value":"2507.14288v1","created_at":"2026-07-05T11:40:03.739037+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.14288","created_at":"2026-07-05T11:40:03.739037+00:00"},{"alias_kind":"pith_short_12","alias_value":"ELFYEDBW4SWT","created_at":"2026-07-05T11:40:03.739037+00:00"},{"alias_kind":"pith_short_16","alias_value":"ELFYEDBW4SWTNMLF","created_at":"2026-07-05T11:40:03.739037+00:00"},{"alias_kind":"pith_short_8","alias_value":"ELFYEDBW","created_at":"2026-07-05T11:40:03.739037+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.29289","citing_title":"Hiding in the Shadow of the Upsilon: Ditaus from a Light Pseudoscalar","ref_index":28,"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":89,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00098","citing_title":"The neutral scalars of type-II 2HDM+S under the LHC","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ELFYEDBW4SWTNMLFNEFPGSW6QE","json":"https://pith.science/pith/ELFYEDBW4SWTNMLFNEFPGSW6QE.json","graph_json":"https://pith.science/api/pith-number/ELFYEDBW4SWTNMLFNEFPGSW6QE/graph.json","events_json":"https://pith.science/api/pith-number/ELFYEDBW4SWTNMLFNEFPGSW6QE/events.json","paper":"https://pith.science/paper/ELFYEDBW"},"agent_actions":{"view_html":"https://pith.science/pith/ELFYEDBW4SWTNMLFNEFPGSW6QE","download_json":"https://pith.science/pith/ELFYEDBW4SWTNMLFNEFPGSW6QE.json","view_paper":"https://pith.science/paper/ELFYEDBW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2507.14288&json=true","fetch_graph":"https://pith.science/api/pith-number/ELFYEDBW4SWTNMLFNEFPGSW6QE/graph.json","fetch_events":"https://pith.science/api/pith-number/ELFYEDBW4SWTNMLFNEFPGSW6QE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ELFYEDBW4SWTNMLFNEFPGSW6QE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ELFYEDBW4SWTNMLFNEFPGSW6QE/action/storage_attestation","attest_author":"https://pith.science/pith/ELFYEDBW4SWTNMLFNEFPGSW6QE/action/author_attestation","sign_citation":"https://pith.science/pith/ELFYEDBW4SWTNMLFNEFPGSW6QE/action/citation_signature","submit_replication":"https://pith.science/pith/ELFYEDBW4SWTNMLFNEFPGSW6QE/action/replication_record"}},"created_at":"2026-07-05T11:40:03.739037+00:00","updated_at":"2026-07-05T11:40:03.739037+00:00"}