{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:VJFXZK7DD4Y5UOJ2DX7KTPTPW3","short_pith_number":"pith:VJFXZK7D","schema_version":"1.0","canonical_sha256":"aa4b7cabe31f31da393a1dfea9be6fb6fa9337245cdebc21457e24b0af38f636","source":{"kind":"arxiv","id":"hep-ph/0504272","version":1},"attestation_state":"computed","paper":{"title":"Dynamical Gauge Symmetry Breaking by Wilson Lines in the Electroweak Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Yutaka Hosotani","submitted_at":"2005-04-28T11:22:46Z","abstract_excerpt":"In higher dimensional gauge theory, dynamics of non-Abelian Aharonov-Bohm phases induces gauge symmetry breaking through the Hosotani mechanism. Higgs fields in the four-dimensional spacetime are identified with the extra-dimensional components of the gauge fields. Basics of the Hosotani mechanism are reviewed, and applied to the electroweak theory. The Higgs boson mass and the Kaluza-Klein excitation scale are related to the weak W-boson mass."},"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":"hep-ph/0504272","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-04-28T11:22:46Z","cross_cats_sorted":[],"title_canon_sha256":"4a2022fe0268e4b8e4660c3dba3bbf01dc0443476793a5ebf8f684ee5ee7efc9","abstract_canon_sha256":"b1835cc86f980df6535811580272eaab3023b56b4b4a5d1838437753cf350c73"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:29:15.298293Z","signature_b64":"YGMWYzML+cSadLv7L0sqBLiHEmmYv7KR8Idf0PWLu7LBzyKnRrqR5ZqmGZY9ulxtlGITels47d07kuTK3rB5DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa4b7cabe31f31da393a1dfea9be6fb6fa9337245cdebc21457e24b0af38f636","last_reissued_at":"2026-07-04T14:29:15.297859Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:29:15.297859Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical Gauge Symmetry Breaking by Wilson Lines in the Electroweak Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Yutaka Hosotani","submitted_at":"2005-04-28T11:22:46Z","abstract_excerpt":"In higher dimensional gauge theory, dynamics of non-Abelian Aharonov-Bohm phases induces gauge symmetry breaking through the Hosotani mechanism. Higgs fields in the four-dimensional spacetime are identified with the extra-dimensional components of the gauge fields. Basics of the Hosotani mechanism are reviewed, and applied to the electroweak theory. The Higgs boson mass and the Kaluza-Klein excitation scale are related to the weak W-boson mass."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0504272","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/hep-ph/0504272/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":"hep-ph/0504272","created_at":"2026-07-04T14:29:15.297917+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0504272v1","created_at":"2026-07-04T14:29:15.297917+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0504272","created_at":"2026-07-04T14:29:15.297917+00:00"},{"alias_kind":"pith_short_12","alias_value":"VJFXZK7DD4Y5","created_at":"2026-07-04T14:29:15.297917+00:00"},{"alias_kind":"pith_short_16","alias_value":"VJFXZK7DD4Y5UOJ2","created_at":"2026-07-04T14:29:15.297917+00:00"},{"alias_kind":"pith_short_8","alias_value":"VJFXZK7D","created_at":"2026-07-04T14:29:15.297917+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.09158","citing_title":"To be, or not to be finite? The Higgs potential in Gauge-Higgs Unification","ref_index":28,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VJFXZK7DD4Y5UOJ2DX7KTPTPW3","json":"https://pith.science/pith/VJFXZK7DD4Y5UOJ2DX7KTPTPW3.json","graph_json":"https://pith.science/api/pith-number/VJFXZK7DD4Y5UOJ2DX7KTPTPW3/graph.json","events_json":"https://pith.science/api/pith-number/VJFXZK7DD4Y5UOJ2DX7KTPTPW3/events.json","paper":"https://pith.science/paper/VJFXZK7D"},"agent_actions":{"view_html":"https://pith.science/pith/VJFXZK7DD4Y5UOJ2DX7KTPTPW3","download_json":"https://pith.science/pith/VJFXZK7DD4Y5UOJ2DX7KTPTPW3.json","view_paper":"https://pith.science/paper/VJFXZK7D","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0504272&json=true","fetch_graph":"https://pith.science/api/pith-number/VJFXZK7DD4Y5UOJ2DX7KTPTPW3/graph.json","fetch_events":"https://pith.science/api/pith-number/VJFXZK7DD4Y5UOJ2DX7KTPTPW3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VJFXZK7DD4Y5UOJ2DX7KTPTPW3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VJFXZK7DD4Y5UOJ2DX7KTPTPW3/action/storage_attestation","attest_author":"https://pith.science/pith/VJFXZK7DD4Y5UOJ2DX7KTPTPW3/action/author_attestation","sign_citation":"https://pith.science/pith/VJFXZK7DD4Y5UOJ2DX7KTPTPW3/action/citation_signature","submit_replication":"https://pith.science/pith/VJFXZK7DD4Y5UOJ2DX7KTPTPW3/action/replication_record"}},"created_at":"2026-07-04T14:29:15.297917+00:00","updated_at":"2026-07-04T14:29:15.297917+00:00"}