{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:ZNMMDECHXSX3TBWZDW6MSSCI4Q","short_pith_number":"pith:ZNMMDECH","schema_version":"1.0","canonical_sha256":"cb58c19047bcafb986d91dbcc94848e42f44b9f7ec96e10420ea34bf8511f2e7","source":{"kind":"arxiv","id":"1902.07726","version":2},"attestation_state":"computed","paper":{"title":"Higgs Parity, Strong CP, and Dark Matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"David Dunsky, Keisuke Harigaya, Lawrence J. Hall","submitted_at":"2019-02-20T19:00:07Z","abstract_excerpt":"An exact spacetime parity replicates the $SU(2) \\times U(1)$ electroweak interaction, the Higgs boson $H$, and the matter of the Standard Model. This \"Higgs Parity\" and the mirror electroweak symmetry are spontaneously broken at scale $v' = \\left\\langle{H'} \\right\\rangle \\gg \\left\\langle{H}\\right\\rangle$, yielding the Standard Model below $v'$ with a quartic coupling that essentially vanishes at $v'$: $\\lambda_{SM}(v') \\sim 10^{-3}$. The strong CP problem is solved as Higgs parity forces the masses of mirror quarks and ordinary quarks to have opposite phases. Dark matter is composed of mirror "},"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":"1902.07726","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-02-20T19:00:07Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"726e1662aca8ab488d60b20ac15e37b6307a94f48f3cd350a87b89753fa86d42","abstract_canon_sha256":"891d12d45c7fde9df13687d7cf67cde16e1025919b788a365dc05a05146b554a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:40:55.434856Z","signature_b64":"fLOWFc6w/W1X8btFnajvz2PW6RZ3TBFfe5rLbP61BS5BxzjcMJ20d8E6hc+tAHHjUmsh8jfa1pIMcfJaI0Q/Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cb58c19047bcafb986d91dbcc94848e42f44b9f7ec96e10420ea34bf8511f2e7","last_reissued_at":"2026-05-17T23:40:55.434094Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:40:55.434094Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs Parity, Strong CP, and Dark Matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"David Dunsky, Keisuke Harigaya, Lawrence J. Hall","submitted_at":"2019-02-20T19:00:07Z","abstract_excerpt":"An exact spacetime parity replicates the $SU(2) \\times U(1)$ electroweak interaction, the Higgs boson $H$, and the matter of the Standard Model. This \"Higgs Parity\" and the mirror electroweak symmetry are spontaneously broken at scale $v' = \\left\\langle{H'} \\right\\rangle \\gg \\left\\langle{H}\\right\\rangle$, yielding the Standard Model below $v'$ with a quartic coupling that essentially vanishes at $v'$: $\\lambda_{SM}(v') \\sim 10^{-3}$. The strong CP problem is solved as Higgs parity forces the masses of mirror quarks and ordinary quarks to have opposite phases. Dark matter is composed of mirror "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.07726","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":"1902.07726","created_at":"2026-05-17T23:40:55.434219+00:00"},{"alias_kind":"arxiv_version","alias_value":"1902.07726v2","created_at":"2026-05-17T23:40:55.434219+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.07726","created_at":"2026-05-17T23:40:55.434219+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZNMMDECHXSX3","created_at":"2026-05-18T12:33:33.725879+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZNMMDECHXSX3TBWZ","created_at":"2026-05-18T12:33:33.725879+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZNMMDECH","created_at":"2026-05-18T12:33:33.725879+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/ZNMMDECHXSX3TBWZDW6MSSCI4Q","json":"https://pith.science/pith/ZNMMDECHXSX3TBWZDW6MSSCI4Q.json","graph_json":"https://pith.science/api/pith-number/ZNMMDECHXSX3TBWZDW6MSSCI4Q/graph.json","events_json":"https://pith.science/api/pith-number/ZNMMDECHXSX3TBWZDW6MSSCI4Q/events.json","paper":"https://pith.science/paper/ZNMMDECH"},"agent_actions":{"view_html":"https://pith.science/pith/ZNMMDECHXSX3TBWZDW6MSSCI4Q","download_json":"https://pith.science/pith/ZNMMDECHXSX3TBWZDW6MSSCI4Q.json","view_paper":"https://pith.science/paper/ZNMMDECH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1902.07726&json=true","fetch_graph":"https://pith.science/api/pith-number/ZNMMDECHXSX3TBWZDW6MSSCI4Q/graph.json","fetch_events":"https://pith.science/api/pith-number/ZNMMDECHXSX3TBWZDW6MSSCI4Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZNMMDECHXSX3TBWZDW6MSSCI4Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZNMMDECHXSX3TBWZDW6MSSCI4Q/action/storage_attestation","attest_author":"https://pith.science/pith/ZNMMDECHXSX3TBWZDW6MSSCI4Q/action/author_attestation","sign_citation":"https://pith.science/pith/ZNMMDECHXSX3TBWZDW6MSSCI4Q/action/citation_signature","submit_replication":"https://pith.science/pith/ZNMMDECHXSX3TBWZDW6MSSCI4Q/action/replication_record"}},"created_at":"2026-05-17T23:40:55.434219+00:00","updated_at":"2026-05-17T23:40:55.434219+00:00"}