{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:4YJE6OFWSLI6MYGU2XJEUDMBIN","short_pith_number":"pith:4YJE6OFW","schema_version":"1.0","canonical_sha256":"e6124f38b692d1e660d4d5d24a0d8143780c7f08afff66d324da2567801951ba","source":{"kind":"arxiv","id":"1403.4775","version":2},"attestation_state":"computed","paper":{"title":"Confronting Higgcision with Electric Dipole Moments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Eibun Senaha, Jae Sik Lee, kingman Cheung, Po-Yan Tseng","submitted_at":"2014-03-19T11:59:36Z","abstract_excerpt":"Current data on the signal strengths and angular spectrum of the 125.5 GeV Higgs boson still allow a CP-mixed state, namely, the pseudoscalar coupling to the top quark can be as sizable as the scalar coupling: $C_u^S \\approx C_u^P =1/2$. CP violation can then arise and manifest in sizable electric dipole moments (EDMs). In the framework of two-Higgs-doublet models, we not only update the Higgs precision (Higgcision) study on the couplings with the most updated Higgs signal strength data, but also compute all the Higgs-mediated contributions from the 125.5 GeV Higgs boson to the EDMs, and confr"},"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":"1403.4775","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-19T11:59:36Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"7979288ff1fd991c7e20b658872f290ef4232ac076823a168c7073283f871901","abstract_canon_sha256":"154c5b4453a8b09cd859e045c0991ee8efadfbefec973aba6d26eec795a1e9e6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:43:59.390036Z","signature_b64":"slTWWU/qRP44OfIjNiUT1HHDOfEcB4lHzvM5LlGB4q7CWW3IC/Gg3Ea2wpjiZnD7WoxUB3zB3hvKKPsjlMaQDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e6124f38b692d1e660d4d5d24a0d8143780c7f08afff66d324da2567801951ba","last_reissued_at":"2026-05-18T01:43:59.389289Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:43:59.389289Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Confronting Higgcision with Electric Dipole Moments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Eibun Senaha, Jae Sik Lee, kingman Cheung, Po-Yan Tseng","submitted_at":"2014-03-19T11:59:36Z","abstract_excerpt":"Current data on the signal strengths and angular spectrum of the 125.5 GeV Higgs boson still allow a CP-mixed state, namely, the pseudoscalar coupling to the top quark can be as sizable as the scalar coupling: $C_u^S \\approx C_u^P =1/2$. CP violation can then arise and manifest in sizable electric dipole moments (EDMs). In the framework of two-Higgs-doublet models, we not only update the Higgs precision (Higgcision) study on the couplings with the most updated Higgs signal strength data, but also compute all the Higgs-mediated contributions from the 125.5 GeV Higgs boson to the EDMs, and confr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.4775","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":"1403.4775","created_at":"2026-05-18T01:43:59.389437+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.4775v2","created_at":"2026-05-18T01:43:59.389437+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.4775","created_at":"2026-05-18T01:43:59.389437+00:00"},{"alias_kind":"pith_short_12","alias_value":"4YJE6OFWSLI6","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_16","alias_value":"4YJE6OFWSLI6MYGU","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_8","alias_value":"4YJE6OFW","created_at":"2026-05-18T12:28:14.216126+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.01318","citing_title":"Gravitational waves from CP domain wall collapse and electron EDM in a complex singlet model with dimension-five Yukawa interactions","ref_index":45,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4YJE6OFWSLI6MYGU2XJEUDMBIN","json":"https://pith.science/pith/4YJE6OFWSLI6MYGU2XJEUDMBIN.json","graph_json":"https://pith.science/api/pith-number/4YJE6OFWSLI6MYGU2XJEUDMBIN/graph.json","events_json":"https://pith.science/api/pith-number/4YJE6OFWSLI6MYGU2XJEUDMBIN/events.json","paper":"https://pith.science/paper/4YJE6OFW"},"agent_actions":{"view_html":"https://pith.science/pith/4YJE6OFWSLI6MYGU2XJEUDMBIN","download_json":"https://pith.science/pith/4YJE6OFWSLI6MYGU2XJEUDMBIN.json","view_paper":"https://pith.science/paper/4YJE6OFW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.4775&json=true","fetch_graph":"https://pith.science/api/pith-number/4YJE6OFWSLI6MYGU2XJEUDMBIN/graph.json","fetch_events":"https://pith.science/api/pith-number/4YJE6OFWSLI6MYGU2XJEUDMBIN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4YJE6OFWSLI6MYGU2XJEUDMBIN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4YJE6OFWSLI6MYGU2XJEUDMBIN/action/storage_attestation","attest_author":"https://pith.science/pith/4YJE6OFWSLI6MYGU2XJEUDMBIN/action/author_attestation","sign_citation":"https://pith.science/pith/4YJE6OFWSLI6MYGU2XJEUDMBIN/action/citation_signature","submit_replication":"https://pith.science/pith/4YJE6OFWSLI6MYGU2XJEUDMBIN/action/replication_record"}},"created_at":"2026-05-18T01:43:59.389437+00:00","updated_at":"2026-05-18T01:43:59.389437+00:00"}