{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:CUDVIKEZFC2JY4KR6L46HOTHEP","short_pith_number":"pith:CUDVIKEZ","schema_version":"1.0","canonical_sha256":"150754289928b49c7151f2f9e3ba6723fc0a12631aa519a0e71464f26f52e8b4","source":{"kind":"arxiv","id":"hep-ph/9604287","version":1},"attestation_state":"computed","paper":{"title":"Scale dependence of quark mass matrices in models with flavor symmetries","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. A. Aguilar-Saavedra, M. Masip","submitted_at":"1996-04-11T18:29:59Z","abstract_excerpt":"Numerical correlations between fermion masses and mixings could indicate the presence of a flavor symmetry at high energies. In general, the search for these correlations using low-energy data requires an estimate of leading-log radiative corrections. We present a complete analysis of the evolution between the electroweak and the grand unification scales of quark mass parameters in minimal supersymmetric models. We take $M_t=180$ GeV and consider all possible values of $\\tan \\beta$. We also analize the possibility that the {\\it top} and/or the {\\it bottom} Yukawa couplings result from an inter"},"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/9604287","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-04-11T18:29:59Z","cross_cats_sorted":[],"title_canon_sha256":"ce51d3cd097b6b1e7b5c17727505057aed648426dcb8a21f7332437fbeffb16f","abstract_canon_sha256":"e4c8b6898f7fcf7fef5bbee11158f83083b6ad86400d233948dab94b838a2f14"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:01:32.616859Z","signature_b64":"AQQNGYDdB4fcz8GKYx3o1pwt9agRs0yhIrQpOWKAd4wYymNMHDecf+id1nYUHAFFXRvsxHY4jZOf5m+p2+KRCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"150754289928b49c7151f2f9e3ba6723fc0a12631aa519a0e71464f26f52e8b4","last_reissued_at":"2026-07-04T16:01:32.616450Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:01:32.616450Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scale dependence of quark mass matrices in models with flavor symmetries","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. A. Aguilar-Saavedra, M. Masip","submitted_at":"1996-04-11T18:29:59Z","abstract_excerpt":"Numerical correlations between fermion masses and mixings could indicate the presence of a flavor symmetry at high energies. In general, the search for these correlations using low-energy data requires an estimate of leading-log radiative corrections. We present a complete analysis of the evolution between the electroweak and the grand unification scales of quark mass parameters in minimal supersymmetric models. We take $M_t=180$ GeV and consider all possible values of $\\tan \\beta$. We also analize the possibility that the {\\it top} and/or the {\\it bottom} Yukawa couplings result from an inter"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9604287","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/9604287/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/9604287","created_at":"2026-07-04T16:01:32.616515+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9604287v1","created_at":"2026-07-04T16:01:32.616515+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9604287","created_at":"2026-07-04T16:01:32.616515+00:00"},{"alias_kind":"pith_short_12","alias_value":"CUDVIKEZFC2J","created_at":"2026-07-04T16:01:32.616515+00:00"},{"alias_kind":"pith_short_16","alias_value":"CUDVIKEZFC2JY4KR","created_at":"2026-07-04T16:01:32.616515+00:00"},{"alias_kind":"pith_short_8","alias_value":"CUDVIKEZ","created_at":"2026-07-04T16:01:32.616515+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/CUDVIKEZFC2JY4KR6L46HOTHEP","json":"https://pith.science/pith/CUDVIKEZFC2JY4KR6L46HOTHEP.json","graph_json":"https://pith.science/api/pith-number/CUDVIKEZFC2JY4KR6L46HOTHEP/graph.json","events_json":"https://pith.science/api/pith-number/CUDVIKEZFC2JY4KR6L46HOTHEP/events.json","paper":"https://pith.science/paper/CUDVIKEZ"},"agent_actions":{"view_html":"https://pith.science/pith/CUDVIKEZFC2JY4KR6L46HOTHEP","download_json":"https://pith.science/pith/CUDVIKEZFC2JY4KR6L46HOTHEP.json","view_paper":"https://pith.science/paper/CUDVIKEZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9604287&json=true","fetch_graph":"https://pith.science/api/pith-number/CUDVIKEZFC2JY4KR6L46HOTHEP/graph.json","fetch_events":"https://pith.science/api/pith-number/CUDVIKEZFC2JY4KR6L46HOTHEP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CUDVIKEZFC2JY4KR6L46HOTHEP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CUDVIKEZFC2JY4KR6L46HOTHEP/action/storage_attestation","attest_author":"https://pith.science/pith/CUDVIKEZFC2JY4KR6L46HOTHEP/action/author_attestation","sign_citation":"https://pith.science/pith/CUDVIKEZFC2JY4KR6L46HOTHEP/action/citation_signature","submit_replication":"https://pith.science/pith/CUDVIKEZFC2JY4KR6L46HOTHEP/action/replication_record"}},"created_at":"2026-07-04T16:01:32.616515+00:00","updated_at":"2026-07-04T16:01:32.616515+00:00"}