{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:ECD7OB6MRH5PM53WKRX3BI7MJH","short_pith_number":"pith:ECD7OB6M","schema_version":"1.0","canonical_sha256":"2087f707cc89faf67776546fb0a3ec49e1848a53bb7421bef9ebfcbac482f705","source":{"kind":"arxiv","id":"hep-ph/0203131","version":3},"attestation_state":"computed","paper":{"title":"Yukawa Quasi-Unification","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Pallis (SISSA), G. Lazarides (Aristotle University of Thessaloniki), Lisbon), M.E. Gomez (IST","submitted_at":"2002-03-14T12:45:06Z","abstract_excerpt":"We construct concrete supersymmetric grand unified theories based on the Pati-Salam gauge group SU(4)_c x SU(2)_L x SU(2)_R which naturally lead to a moderate violation of \"asymptotic\" Yukawa unification and thus can allow an acceptable b-quark mass even with universal boundary conditions. We consider the constrained minimal supersymmetric standard model which emerges from one of these theories with a deviation from Yukawa unification which is adequate for mu>0. We show that this model possesses a wide and natural range of parameters which is consistent with the data on b --> s gamma, the muon"},"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/0203131","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-03-14T12:45:06Z","cross_cats_sorted":[],"title_canon_sha256":"d03b15f3e63012537cbf40a64fb044563d4633d4d6702819a782f566b91987c6","abstract_canon_sha256":"44c7bd3d6f3880d8c6881894fd2c0ce1b4953d6c856fd980cc0f151109cdf0fe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:26:41.945973Z","signature_b64":"g3jebOaePvHCWCyOnLygx719HzAg1YWWVJUkMtPdFN1BeP/3zl01tHYnzi17ONcutlc0XhuBXg1UklZDkIT8Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2087f707cc89faf67776546fb0a3ec49e1848a53bb7421bef9ebfcbac482f705","last_reissued_at":"2026-07-04T15:26:41.945560Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:26:41.945560Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Yukawa Quasi-Unification","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Pallis (SISSA), G. Lazarides (Aristotle University of Thessaloniki), Lisbon), M.E. Gomez (IST","submitted_at":"2002-03-14T12:45:06Z","abstract_excerpt":"We construct concrete supersymmetric grand unified theories based on the Pati-Salam gauge group SU(4)_c x SU(2)_L x SU(2)_R which naturally lead to a moderate violation of \"asymptotic\" Yukawa unification and thus can allow an acceptable b-quark mass even with universal boundary conditions. We consider the constrained minimal supersymmetric standard model which emerges from one of these theories with a deviation from Yukawa unification which is adequate for mu>0. We show that this model possesses a wide and natural range of parameters which is consistent with the data on b --> s gamma, the muon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0203131","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/0203131/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/0203131","created_at":"2026-07-04T15:26:41.945619+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0203131v3","created_at":"2026-07-04T15:26:41.945619+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0203131","created_at":"2026-07-04T15:26:41.945619+00:00"},{"alias_kind":"pith_short_12","alias_value":"ECD7OB6MRH5P","created_at":"2026-07-04T15:26:41.945619+00:00"},{"alias_kind":"pith_short_16","alias_value":"ECD7OB6MRH5PM53W","created_at":"2026-07-04T15:26:41.945619+00:00"},{"alias_kind":"pith_short_8","alias_value":"ECD7OB6M","created_at":"2026-07-04T15:26:41.945619+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.11806","citing_title":"Fermion masses and mixings in supersymmetric SO(10) with third-generation quasi-Yukawa unification","ref_index":10,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ECD7OB6MRH5PM53WKRX3BI7MJH","json":"https://pith.science/pith/ECD7OB6MRH5PM53WKRX3BI7MJH.json","graph_json":"https://pith.science/api/pith-number/ECD7OB6MRH5PM53WKRX3BI7MJH/graph.json","events_json":"https://pith.science/api/pith-number/ECD7OB6MRH5PM53WKRX3BI7MJH/events.json","paper":"https://pith.science/paper/ECD7OB6M"},"agent_actions":{"view_html":"https://pith.science/pith/ECD7OB6MRH5PM53WKRX3BI7MJH","download_json":"https://pith.science/pith/ECD7OB6MRH5PM53WKRX3BI7MJH.json","view_paper":"https://pith.science/paper/ECD7OB6M","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0203131&json=true","fetch_graph":"https://pith.science/api/pith-number/ECD7OB6MRH5PM53WKRX3BI7MJH/graph.json","fetch_events":"https://pith.science/api/pith-number/ECD7OB6MRH5PM53WKRX3BI7MJH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ECD7OB6MRH5PM53WKRX3BI7MJH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ECD7OB6MRH5PM53WKRX3BI7MJH/action/storage_attestation","attest_author":"https://pith.science/pith/ECD7OB6MRH5PM53WKRX3BI7MJH/action/author_attestation","sign_citation":"https://pith.science/pith/ECD7OB6MRH5PM53WKRX3BI7MJH/action/citation_signature","submit_replication":"https://pith.science/pith/ECD7OB6MRH5PM53WKRX3BI7MJH/action/replication_record"}},"created_at":"2026-07-04T15:26:41.945619+00:00","updated_at":"2026-07-04T15:26:41.945619+00:00"}