{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:K7CKMGOB3655UWR4WNZ4AXTZUX","short_pith_number":"pith:K7CKMGOB","schema_version":"1.0","canonical_sha256":"57c4a619c1dfbbda5a3cb373c05e79a5e149a89c9f53c790938468ac09112ca0","source":{"kind":"arxiv","id":"hep-ph/0607064","version":1},"attestation_state":"computed","paper":{"title":"All-order Finiteness of the Higgs Boson Mass in the Dynamical Gauge-Higgs Unification","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Yutaka Hosotani","submitted_at":"2006-07-06T10:47:48Z","abstract_excerpt":"In the dynamical gauge-Higgs unification, it is shown that the mass of the Higgs boson (4D scalar field) in U(1) gauge theory in $M^4 \\times T^n$ ($n=1,2,3,...$) is finite to all order in perturbation theory as a consequence of the large gauge invariance. It is conjectured that the Higgs boson mass is finite in non-Abelian gauge theory in $M^4 \\times S^1$, $M^4 \\times (S^1/Z_2)$ and the Randall-Sundrum warped spacetime to all order in the rearranged perturbation theory where the large gauge invariance is maintained."},"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/0607064","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-07-06T10:47:48Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"2c081adeacff42b85d594ed997615f7d8fe99d5c51dcdabb1804a02208986167","abstract_canon_sha256":"6fc7e781742b48104c3c4340c063505f807fdc5b5974c4bacc9cf85f33a02c9a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:55:27.485029Z","signature_b64":"h6BeCTjoSUXtgs2vzJ9c67yzmQl9lwUw6QRzBBKRvwJkPh17rcMlrkRi9QSlx1yBr7DCwxWUc0D4zqRBUUglAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"57c4a619c1dfbbda5a3cb373c05e79a5e149a89c9f53c790938468ac09112ca0","last_reissued_at":"2026-07-04T14:55:27.484603Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:55:27.484603Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"All-order Finiteness of the Higgs Boson Mass in the Dynamical Gauge-Higgs Unification","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Yutaka Hosotani","submitted_at":"2006-07-06T10:47:48Z","abstract_excerpt":"In the dynamical gauge-Higgs unification, it is shown that the mass of the Higgs boson (4D scalar field) in U(1) gauge theory in $M^4 \\times T^n$ ($n=1,2,3,...$) is finite to all order in perturbation theory as a consequence of the large gauge invariance. It is conjectured that the Higgs boson mass is finite in non-Abelian gauge theory in $M^4 \\times S^1$, $M^4 \\times (S^1/Z_2)$ and the Randall-Sundrum warped spacetime to all order in the rearranged perturbation theory where the large gauge invariance is maintained."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0607064","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/0607064/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/0607064","created_at":"2026-07-04T14:55:27.484666+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0607064v1","created_at":"2026-07-04T14:55:27.484666+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0607064","created_at":"2026-07-04T14:55:27.484666+00:00"},{"alias_kind":"pith_short_12","alias_value":"K7CKMGOB3655","created_at":"2026-07-04T14:55:27.484666+00:00"},{"alias_kind":"pith_short_16","alias_value":"K7CKMGOB3655UWR4","created_at":"2026-07-04T14:55:27.484666+00:00"},{"alias_kind":"pith_short_8","alias_value":"K7CKMGOB","created_at":"2026-07-04T14:55:27.484666+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.22119","citing_title":"Massless limit of massive self-interacting vector fields","ref_index":17,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K7CKMGOB3655UWR4WNZ4AXTZUX","json":"https://pith.science/pith/K7CKMGOB3655UWR4WNZ4AXTZUX.json","graph_json":"https://pith.science/api/pith-number/K7CKMGOB3655UWR4WNZ4AXTZUX/graph.json","events_json":"https://pith.science/api/pith-number/K7CKMGOB3655UWR4WNZ4AXTZUX/events.json","paper":"https://pith.science/paper/K7CKMGOB"},"agent_actions":{"view_html":"https://pith.science/pith/K7CKMGOB3655UWR4WNZ4AXTZUX","download_json":"https://pith.science/pith/K7CKMGOB3655UWR4WNZ4AXTZUX.json","view_paper":"https://pith.science/paper/K7CKMGOB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0607064&json=true","fetch_graph":"https://pith.science/api/pith-number/K7CKMGOB3655UWR4WNZ4AXTZUX/graph.json","fetch_events":"https://pith.science/api/pith-number/K7CKMGOB3655UWR4WNZ4AXTZUX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K7CKMGOB3655UWR4WNZ4AXTZUX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K7CKMGOB3655UWR4WNZ4AXTZUX/action/storage_attestation","attest_author":"https://pith.science/pith/K7CKMGOB3655UWR4WNZ4AXTZUX/action/author_attestation","sign_citation":"https://pith.science/pith/K7CKMGOB3655UWR4WNZ4AXTZUX/action/citation_signature","submit_replication":"https://pith.science/pith/K7CKMGOB3655UWR4WNZ4AXTZUX/action/replication_record"}},"created_at":"2026-07-04T14:55:27.484666+00:00","updated_at":"2026-07-04T14:55:27.484666+00:00"}