{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:MUAUMXOADL2TIEMI624K5ONOGI","short_pith_number":"pith:MUAUMXOA","schema_version":"1.0","canonical_sha256":"6501465dc01af5341188f6b8aeb9ae32256d75a743ae8ea1a03caec305038c7c","source":{"kind":"arxiv","id":"hep-ph/0212035","version":3},"attestation_state":"computed","paper":{"title":"Dynamical Rearrangement of Gauge Symmetry on the Orbifold S^1/Z_2","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Masatomi Harada, Naoyuki Haba, Yoshiharu Kawamura, Yutaka Hosotani","submitted_at":"2002-12-03T08:45:20Z","abstract_excerpt":"Gauge theory defined on the orbifold $M^4 \\times (S^1/Z_2)$ is investigated from the viewpoint of the Hosotani mechanism. Rearrangement of gauge symmetry takes place due to the dynamics of Wilson line phases. The physical symmetry of the theory, in general, differs from the symmetry of the boundary conditions. Several sets of boundary conditions having distinct symmetry can be related by gauge transformations, belonging to the same equivalence class. The Hosotani mechanism guarantees the same physics in all theories in one equivalent class. Examples are presented in the SU(5) theory. Zero mode"},"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/0212035","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-12-03T08:45:20Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"51ace24a5c344ec26b2b8ce67f6006d2a63fb3027b0dbba3cc9dc6da2ae92dc7","abstract_canon_sha256":"a414c2073c67c173b3f3f8ba775fb45e5325cb85764b1edc2e985ab66bfed7b9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:04:42.861033Z","signature_b64":"swiUDOr3ONNWysCyFCfh4EcOLu8vNiywis1Q+hQ6vCv88sbL8hBw/k2zFzXDvXQn1AIGYdiA9tvXfcGCBh/gDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6501465dc01af5341188f6b8aeb9ae32256d75a743ae8ea1a03caec305038c7c","last_reissued_at":"2026-05-18T04:04:42.860579Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:04:42.860579Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical Rearrangement of Gauge Symmetry on the Orbifold S^1/Z_2","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Masatomi Harada, Naoyuki Haba, Yoshiharu Kawamura, Yutaka Hosotani","submitted_at":"2002-12-03T08:45:20Z","abstract_excerpt":"Gauge theory defined on the orbifold $M^4 \\times (S^1/Z_2)$ is investigated from the viewpoint of the Hosotani mechanism. Rearrangement of gauge symmetry takes place due to the dynamics of Wilson line phases. The physical symmetry of the theory, in general, differs from the symmetry of the boundary conditions. Several sets of boundary conditions having distinct symmetry can be related by gauge transformations, belonging to the same equivalence class. The Hosotani mechanism guarantees the same physics in all theories in one equivalent class. Examples are presented in the SU(5) theory. Zero mode"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0212035","kind":"arxiv","version":3},"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":"hep-ph/0212035","created_at":"2026-05-18T04:04:42.860640+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0212035v3","created_at":"2026-05-18T04:04:42.860640+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0212035","created_at":"2026-05-18T04:04:42.860640+00:00"},{"alias_kind":"pith_short_12","alias_value":"MUAUMXOADL2T","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_16","alias_value":"MUAUMXOADL2TIEMI","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_8","alias_value":"MUAUMXOA","created_at":"2026-05-18T12:25:51.375804+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/MUAUMXOADL2TIEMI624K5ONOGI","json":"https://pith.science/pith/MUAUMXOADL2TIEMI624K5ONOGI.json","graph_json":"https://pith.science/api/pith-number/MUAUMXOADL2TIEMI624K5ONOGI/graph.json","events_json":"https://pith.science/api/pith-number/MUAUMXOADL2TIEMI624K5ONOGI/events.json","paper":"https://pith.science/paper/MUAUMXOA"},"agent_actions":{"view_html":"https://pith.science/pith/MUAUMXOADL2TIEMI624K5ONOGI","download_json":"https://pith.science/pith/MUAUMXOADL2TIEMI624K5ONOGI.json","view_paper":"https://pith.science/paper/MUAUMXOA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0212035&json=true","fetch_graph":"https://pith.science/api/pith-number/MUAUMXOADL2TIEMI624K5ONOGI/graph.json","fetch_events":"https://pith.science/api/pith-number/MUAUMXOADL2TIEMI624K5ONOGI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MUAUMXOADL2TIEMI624K5ONOGI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MUAUMXOADL2TIEMI624K5ONOGI/action/storage_attestation","attest_author":"https://pith.science/pith/MUAUMXOADL2TIEMI624K5ONOGI/action/author_attestation","sign_citation":"https://pith.science/pith/MUAUMXOADL2TIEMI624K5ONOGI/action/citation_signature","submit_replication":"https://pith.science/pith/MUAUMXOADL2TIEMI624K5ONOGI/action/replication_record"}},"created_at":"2026-05-18T04:04:42.860640+00:00","updated_at":"2026-05-18T04:04:42.860640+00:00"}