{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:WHKS76CTDHOSZYTXHNQ7SHICFJ","short_pith_number":"pith:WHKS76CT","schema_version":"1.0","canonical_sha256":"b1d52ff85319dd2ce2773b61f91d022a50ec6d59124371e066715231cd4317f7","source":{"kind":"arxiv","id":"hep-ph/0206021","version":2},"attestation_state":"computed","paper":{"title":"The Littlest Higgs","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A.E. Nelson, A.G. Cohen, E. Katz, N. Arkani-Hamed","submitted_at":"2002-06-03T20:20:23Z","abstract_excerpt":"We present an economical theory of natural electroweak symmetry breaking, generalizing an approach based on deconstruction. This theory is the smallest extension of the Standard Model to date that stabilizes the electroweak scale with a naturally light Higgs and weakly coupled new physics at TeV energies. The Higgs is one of a set of pseudo Goldstone bosons in an $SU(5)/SO(5)$ nonlinear sigma model. The symmetry breaking scale $f$ is around a TeV, with the cutoff $\\Lambda \\lsim 4\\pi f \\sim $ 10 TeV. A single electroweak doublet, the ``little Higgs'', is automatically much lighter than the othe"},"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/0206021","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-06-03T20:20:23Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"d2d70a2041cc32749e9322d7d3c8393625c430c88536b26cda3ac8a1c6ad17af","abstract_canon_sha256":"a9f2f201650d7be47ccf2a849d86ac27e1b704a41ddad24fd378eff4e04ecbad"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:31:42.899474Z","signature_b64":"wP8ZpW1HQzuBLg8h6nB+svHUxNkAJM8U62BV9p9tHZkJTrt5fMDvmK+F17stRJMdc7/o79uT3ALDBGVbw7oKDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b1d52ff85319dd2ce2773b61f91d022a50ec6d59124371e066715231cd4317f7","last_reissued_at":"2026-05-18T04:31:42.899088Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:31:42.899088Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Littlest Higgs","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A.E. Nelson, A.G. Cohen, E. Katz, N. Arkani-Hamed","submitted_at":"2002-06-03T20:20:23Z","abstract_excerpt":"We present an economical theory of natural electroweak symmetry breaking, generalizing an approach based on deconstruction. This theory is the smallest extension of the Standard Model to date that stabilizes the electroweak scale with a naturally light Higgs and weakly coupled new physics at TeV energies. The Higgs is one of a set of pseudo Goldstone bosons in an $SU(5)/SO(5)$ nonlinear sigma model. The symmetry breaking scale $f$ is around a TeV, with the cutoff $\\Lambda \\lsim 4\\pi f \\sim $ 10 TeV. A single electroweak doublet, the ``little Higgs'', is automatically much lighter than the othe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0206021","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":"hep-ph/0206021","created_at":"2026-05-18T04:31:42.899144+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0206021v2","created_at":"2026-05-18T04:31:42.899144+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0206021","created_at":"2026-05-18T04:31:42.899144+00:00"},{"alias_kind":"pith_short_12","alias_value":"WHKS76CTDHOS","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_16","alias_value":"WHKS76CTDHOSZYTX","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_8","alias_value":"WHKS76CT","created_at":"2026-05-18T12:25:51.375804+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.20848","citing_title":"Confronting Vector-Like Quark Models with LHC Searches","ref_index":7,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WHKS76CTDHOSZYTXHNQ7SHICFJ","json":"https://pith.science/pith/WHKS76CTDHOSZYTXHNQ7SHICFJ.json","graph_json":"https://pith.science/api/pith-number/WHKS76CTDHOSZYTXHNQ7SHICFJ/graph.json","events_json":"https://pith.science/api/pith-number/WHKS76CTDHOSZYTXHNQ7SHICFJ/events.json","paper":"https://pith.science/paper/WHKS76CT"},"agent_actions":{"view_html":"https://pith.science/pith/WHKS76CTDHOSZYTXHNQ7SHICFJ","download_json":"https://pith.science/pith/WHKS76CTDHOSZYTXHNQ7SHICFJ.json","view_paper":"https://pith.science/paper/WHKS76CT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0206021&json=true","fetch_graph":"https://pith.science/api/pith-number/WHKS76CTDHOSZYTXHNQ7SHICFJ/graph.json","fetch_events":"https://pith.science/api/pith-number/WHKS76CTDHOSZYTXHNQ7SHICFJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WHKS76CTDHOSZYTXHNQ7SHICFJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WHKS76CTDHOSZYTXHNQ7SHICFJ/action/storage_attestation","attest_author":"https://pith.science/pith/WHKS76CTDHOSZYTXHNQ7SHICFJ/action/author_attestation","sign_citation":"https://pith.science/pith/WHKS76CTDHOSZYTXHNQ7SHICFJ/action/citation_signature","submit_replication":"https://pith.science/pith/WHKS76CTDHOSZYTXHNQ7SHICFJ/action/replication_record"}},"created_at":"2026-05-18T04:31:42.899144+00:00","updated_at":"2026-05-18T04:31:42.899144+00:00"}