{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:TLN7WM6UVPOCG27FTCQQCK373A","short_pith_number":"pith:TLN7WM6U","schema_version":"1.0","canonical_sha256":"9adbfb33d4abdc236be598a1012b7fd81e9274d941a475832219d4cd9b023195","source":{"kind":"arxiv","id":"1803.07271","version":2},"attestation_state":"computed","paper":{"title":"Dynamical Gauge Boson of Hidden Local Symmetry within the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Koichi Yamawaki","submitted_at":"2018-03-20T06:22:41Z","abstract_excerpt":"The Standard Model (SM) Higgs Lagrangian is straightforwardly rewritten into the {\\it scale-invariant} nonlinear sigma model $G/H=[SU(2)_L \\times SU(2)_R]/SU(2)_{V}\\simeq O(4)/O(3)$, with the (approximate) scale symmetry realized nonlinearly by the (pseudo) dilaton ($=$ SM Higgs). It is further gauge equivalent to that having the symmetry $O(4)_{\\rm global}\\times O(3)_{\\rm local}$, with $O(3)_{\\rm local}$ being the Hidden Local Symmetry (HLS). In the large $N$ limit of the scale-invariant version of the Grassmannian model $G/H=O(N)/[O(N-3)\\times O(3)] $ $\\simeq O(N)_{\\rm global}\\times [O(N-3)\\"},"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":"1803.07271","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-03-20T06:22:41Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"259425e98c88c0903245c8af483495b7e67cb00ebffa236734e94539d385c393","abstract_canon_sha256":"611a340bead5b6ff759015aa4e65e01430cdcb31b27fd8a3c3668c30fa471adb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:10:38.187715Z","signature_b64":"60p/6Yfk1HkiCwXnkuddVhm1y0Bs5Sey8PYXssV5fUDgJ5riP6WbRCH/9vgBf6JcHCLk+zCXp0B8l0tbGblNCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9adbfb33d4abdc236be598a1012b7fd81e9274d941a475832219d4cd9b023195","last_reissued_at":"2026-05-18T00:10:38.186993Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:10:38.186993Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical Gauge Boson of Hidden Local Symmetry within the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Koichi Yamawaki","submitted_at":"2018-03-20T06:22:41Z","abstract_excerpt":"The Standard Model (SM) Higgs Lagrangian is straightforwardly rewritten into the {\\it scale-invariant} nonlinear sigma model $G/H=[SU(2)_L \\times SU(2)_R]/SU(2)_{V}\\simeq O(4)/O(3)$, with the (approximate) scale symmetry realized nonlinearly by the (pseudo) dilaton ($=$ SM Higgs). It is further gauge equivalent to that having the symmetry $O(4)_{\\rm global}\\times O(3)_{\\rm local}$, with $O(3)_{\\rm local}$ being the Hidden Local Symmetry (HLS). In the large $N$ limit of the scale-invariant version of the Grassmannian model $G/H=O(N)/[O(N-3)\\times O(3)] $ $\\simeq O(N)_{\\rm global}\\times [O(N-3)\\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.07271","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":"1803.07271","created_at":"2026-05-18T00:10:38.187114+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.07271v2","created_at":"2026-05-18T00:10:38.187114+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.07271","created_at":"2026-05-18T00:10:38.187114+00:00"},{"alias_kind":"pith_short_12","alias_value":"TLN7WM6UVPOC","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_16","alias_value":"TLN7WM6UVPOCG27F","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_8","alias_value":"TLN7WM6U","created_at":"2026-05-18T12:32:53.628368+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/TLN7WM6UVPOCG27FTCQQCK373A","json":"https://pith.science/pith/TLN7WM6UVPOCG27FTCQQCK373A.json","graph_json":"https://pith.science/api/pith-number/TLN7WM6UVPOCG27FTCQQCK373A/graph.json","events_json":"https://pith.science/api/pith-number/TLN7WM6UVPOCG27FTCQQCK373A/events.json","paper":"https://pith.science/paper/TLN7WM6U"},"agent_actions":{"view_html":"https://pith.science/pith/TLN7WM6UVPOCG27FTCQQCK373A","download_json":"https://pith.science/pith/TLN7WM6UVPOCG27FTCQQCK373A.json","view_paper":"https://pith.science/paper/TLN7WM6U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.07271&json=true","fetch_graph":"https://pith.science/api/pith-number/TLN7WM6UVPOCG27FTCQQCK373A/graph.json","fetch_events":"https://pith.science/api/pith-number/TLN7WM6UVPOCG27FTCQQCK373A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TLN7WM6UVPOCG27FTCQQCK373A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TLN7WM6UVPOCG27FTCQQCK373A/action/storage_attestation","attest_author":"https://pith.science/pith/TLN7WM6UVPOCG27FTCQQCK373A/action/author_attestation","sign_citation":"https://pith.science/pith/TLN7WM6UVPOCG27FTCQQCK373A/action/citation_signature","submit_replication":"https://pith.science/pith/TLN7WM6UVPOCG27FTCQQCK373A/action/replication_record"}},"created_at":"2026-05-18T00:10:38.187114+00:00","updated_at":"2026-05-18T00:10:38.187114+00:00"}