{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:6NHIIC2SJBJV5AVS7BDNQCWDIF","short_pith_number":"pith:6NHIIC2S","schema_version":"1.0","canonical_sha256":"f34e840b5248535e82b2f846d80ac34141764753646508f4799e72cf85d7ecc7","source":{"kind":"arxiv","id":"hep-ph/0502182","version":1},"attestation_state":"computed","paper":{"title":"Little Higgs Review","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David Tucker-Smith, Martin Schmaltz","submitted_at":"2005-02-19T23:44:32Z","abstract_excerpt":"Recently there has been renewed interest in the possibility that the Higgs particle of the Standard Model is a pseudo-Nambu-Goldstone boson. This development was spurred by the observation that if certain global symmetries are broken only by the interplay between two or more coupling constants, then the Higgs mass-squared is free from quadratic divergences at one loop. This \"collective symmetry\" breaking is the essential ingredient in little Higgs theories, which are weakly coupled extensions of the Standard Model with little or no fine tuning, describing physics up to an energy scale ~10 TeV."},"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/0502182","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-02-19T23:44:32Z","cross_cats_sorted":[],"title_canon_sha256":"8137933eee90d8f393272fdf0aa6ae4b21cdddcba01cb390cd4a02e1c5a8ef56","abstract_canon_sha256":"d3c511231a7b12fc69079b434cd4edea7c7ce23af8752b6bbe0b5b945ff2360b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:55:30.288216Z","signature_b64":"lq7nHFE1x0AgrBO0ENhWbjEgv5/qZSuEWWHwSu7nHimB94O5DA4vWBPUINAzX9YtgixJblVclqdXM3kTVCOfCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f34e840b5248535e82b2f846d80ac34141764753646508f4799e72cf85d7ecc7","last_reissued_at":"2026-07-04T16:55:30.287880Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:55:30.287880Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Little Higgs Review","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David Tucker-Smith, Martin Schmaltz","submitted_at":"2005-02-19T23:44:32Z","abstract_excerpt":"Recently there has been renewed interest in the possibility that the Higgs particle of the Standard Model is a pseudo-Nambu-Goldstone boson. This development was spurred by the observation that if certain global symmetries are broken only by the interplay between two or more coupling constants, then the Higgs mass-squared is free from quadratic divergences at one loop. This \"collective symmetry\" breaking is the essential ingredient in little Higgs theories, which are weakly coupled extensions of the Standard Model with little or no fine tuning, describing physics up to an energy scale ~10 TeV."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0502182","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/0502182/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/0502182","created_at":"2026-07-04T16:55:30.287938+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0502182v1","created_at":"2026-07-04T16:55:30.287938+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0502182","created_at":"2026-07-04T16:55:30.287938+00:00"},{"alias_kind":"pith_short_12","alias_value":"6NHIIC2SJBJV","created_at":"2026-07-04T16:55:30.287938+00:00"},{"alias_kind":"pith_short_16","alias_value":"6NHIIC2SJBJV5AVS","created_at":"2026-07-04T16:55:30.287938+00:00"},{"alias_kind":"pith_short_8","alias_value":"6NHIIC2S","created_at":"2026-07-04T16:55:30.287938+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.28538","citing_title":"Search for pair-produced vector-like $T$-quarks decaying into $Ht$ final states in the lepton-plus-jets channel in $pp$ collisions at $\\sqrt{s}$=13 TeV with the ATLAS detector","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2605.20848","citing_title":"VLQBounds: Confronting Vector-Like Quark Models with LHC Searches","ref_index":8,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6NHIIC2SJBJV5AVS7BDNQCWDIF","json":"https://pith.science/pith/6NHIIC2SJBJV5AVS7BDNQCWDIF.json","graph_json":"https://pith.science/api/pith-number/6NHIIC2SJBJV5AVS7BDNQCWDIF/graph.json","events_json":"https://pith.science/api/pith-number/6NHIIC2SJBJV5AVS7BDNQCWDIF/events.json","paper":"https://pith.science/paper/6NHIIC2S"},"agent_actions":{"view_html":"https://pith.science/pith/6NHIIC2SJBJV5AVS7BDNQCWDIF","download_json":"https://pith.science/pith/6NHIIC2SJBJV5AVS7BDNQCWDIF.json","view_paper":"https://pith.science/paper/6NHIIC2S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0502182&json=true","fetch_graph":"https://pith.science/api/pith-number/6NHIIC2SJBJV5AVS7BDNQCWDIF/graph.json","fetch_events":"https://pith.science/api/pith-number/6NHIIC2SJBJV5AVS7BDNQCWDIF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6NHIIC2SJBJV5AVS7BDNQCWDIF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6NHIIC2SJBJV5AVS7BDNQCWDIF/action/storage_attestation","attest_author":"https://pith.science/pith/6NHIIC2SJBJV5AVS7BDNQCWDIF/action/author_attestation","sign_citation":"https://pith.science/pith/6NHIIC2SJBJV5AVS7BDNQCWDIF/action/citation_signature","submit_replication":"https://pith.science/pith/6NHIIC2SJBJV5AVS7BDNQCWDIF/action/replication_record"}},"created_at":"2026-07-04T16:55:30.287938+00:00","updated_at":"2026-07-04T16:55:30.287938+00:00"}