{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:L6A27DHT5D3BMSZTW5CASJOAWP","short_pith_number":"pith:L6A27DHT","schema_version":"1.0","canonical_sha256":"5f81af8cf3e8f6164b33b7440925c0b3f4d7440208ab88f8563d3e8866ebfed7","source":{"kind":"arxiv","id":"hep-ph/9702416","version":3},"attestation_state":"computed","paper":{"title":"Flavor Physics and the Triviality Bound on the Higgs Mass","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"B. A. Dobrescu, E. H. Simmons, R. S. Chivukula","submitted_at":"1997-02-25T13:50:11Z","abstract_excerpt":"The triviality of the scalar sector of the standard one-doublet Higgs model implies that this model is only an effective low-energy theory valid below some cut-off scale $\\Lambda$. The underlying high-energy theory must include flavor dynamics at a scale of order $\\Lambda$ or greater in order to give rise to the different Yukawa couplings of the Higgs to ordinary fermions. This flavor dynamics will generically produce flavor-changing neutral currents and non-universal corrections to Z -> b b-bar. We show that the experimental constraints on the neutral D-meson mass difference imply that $\\Lamb"},"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/9702416","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-02-25T13:50:11Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"4ac40f06885f8bc3ae04a01dbdc56a83b505adcbb92746633c0243190f0668b4","abstract_canon_sha256":"9f9e500aaf832aaa9710a1efaaea721590e7d3424ce60fa2f62f581405a39f1c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:32:24.758756Z","signature_b64":"QSoDZ9W+88XoDaUdGBs4xWxjkj4jGpEyxX3uep3lUIklM7SptB9P7lWEXqTU03B3D+h9cqGqmQtqUGuLsITQAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5f81af8cf3e8f6164b33b7440925c0b3f4d7440208ab88f8563d3e8866ebfed7","last_reissued_at":"2026-07-04T15:32:24.758235Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:32:24.758235Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Flavor Physics and the Triviality Bound on the Higgs Mass","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"B. A. Dobrescu, E. H. Simmons, R. S. Chivukula","submitted_at":"1997-02-25T13:50:11Z","abstract_excerpt":"The triviality of the scalar sector of the standard one-doublet Higgs model implies that this model is only an effective low-energy theory valid below some cut-off scale $\\Lambda$. The underlying high-energy theory must include flavor dynamics at a scale of order $\\Lambda$ or greater in order to give rise to the different Yukawa couplings of the Higgs to ordinary fermions. This flavor dynamics will generically produce flavor-changing neutral currents and non-universal corrections to Z -> b b-bar. We show that the experimental constraints on the neutral D-meson mass difference imply that $\\Lamb"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9702416","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9702416/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/9702416","created_at":"2026-07-04T15:32:24.758380+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9702416v3","created_at":"2026-07-04T15:32:24.758380+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9702416","created_at":"2026-07-04T15:32:24.758380+00:00"},{"alias_kind":"pith_short_12","alias_value":"L6A27DHT5D3B","created_at":"2026-07-04T15:32:24.758380+00:00"},{"alias_kind":"pith_short_16","alias_value":"L6A27DHT5D3BMSZT","created_at":"2026-07-04T15:32:24.758380+00:00"},{"alias_kind":"pith_short_8","alias_value":"L6A27DHT","created_at":"2026-07-04T15:32:24.758380+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/L6A27DHT5D3BMSZTW5CASJOAWP","json":"https://pith.science/pith/L6A27DHT5D3BMSZTW5CASJOAWP.json","graph_json":"https://pith.science/api/pith-number/L6A27DHT5D3BMSZTW5CASJOAWP/graph.json","events_json":"https://pith.science/api/pith-number/L6A27DHT5D3BMSZTW5CASJOAWP/events.json","paper":"https://pith.science/paper/L6A27DHT"},"agent_actions":{"view_html":"https://pith.science/pith/L6A27DHT5D3BMSZTW5CASJOAWP","download_json":"https://pith.science/pith/L6A27DHT5D3BMSZTW5CASJOAWP.json","view_paper":"https://pith.science/paper/L6A27DHT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9702416&json=true","fetch_graph":"https://pith.science/api/pith-number/L6A27DHT5D3BMSZTW5CASJOAWP/graph.json","fetch_events":"https://pith.science/api/pith-number/L6A27DHT5D3BMSZTW5CASJOAWP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L6A27DHT5D3BMSZTW5CASJOAWP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L6A27DHT5D3BMSZTW5CASJOAWP/action/storage_attestation","attest_author":"https://pith.science/pith/L6A27DHT5D3BMSZTW5CASJOAWP/action/author_attestation","sign_citation":"https://pith.science/pith/L6A27DHT5D3BMSZTW5CASJOAWP/action/citation_signature","submit_replication":"https://pith.science/pith/L6A27DHT5D3BMSZTW5CASJOAWP/action/replication_record"}},"created_at":"2026-07-04T15:32:24.758380+00:00","updated_at":"2026-07-04T15:32:24.758380+00:00"}