{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:SCQZUMYZXITTNTC7NS2AWKC5AI","short_pith_number":"pith:SCQZUMYZ","schema_version":"1.0","canonical_sha256":"90a19a3319ba2736cc5f6cb40b285d021c338a72529efb248a7fa74b4b52ae18","source":{"kind":"arxiv","id":"1111.3639","version":1},"attestation_state":"computed","paper":{"title":"An Alternative Yukawa Unified SUSY Scenario","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Carlos E. M. Wagner, James S. Gainer, Ran Huo","submitted_at":"2011-11-15T21:00:02Z","abstract_excerpt":"Supersymmetric SO(10) Grand Unified Theories with Yukawa unification represent an appealing possibility for physics beyond the Standard Model. However Yukawa unification is made difficult by large threshold corrections to the bottom mass. Generally one is led to consider models where the sfermion masses are large in order to suppress these corrections. Here we present another possibility, in which the top and bottom GUT scale Yukawa couplings are equal to a component of the charged lepton Yukawa matrix at the GUT scale in a basis where this matrix is not diagonal. Physically, this weak eigenst"},"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":"1111.3639","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-11-15T21:00:02Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"84f2cb8a3ebeea15fef8b4c854cb49581c8ad2e2bf62bd0350b563628d7ff7ae","abstract_canon_sha256":"a7a3d74aff2dff608eab20a1957a2721fcb5f5aebdc39b20fc5d576c68eac00a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:32.775957Z","signature_b64":"56z5uXhtHYNFZ7Fwf8r69AY1NbiW+pJoqjEXIV2pieIZy//i2MX/0Jo4//ZNDtmBVeok5m7aidJJc3/5iIY2Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"90a19a3319ba2736cc5f6cb40b285d021c338a72529efb248a7fa74b4b52ae18","last_reissued_at":"2026-05-18T01:59:32.775282Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:32.775282Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An Alternative Yukawa Unified SUSY Scenario","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Carlos E. M. Wagner, James S. Gainer, Ran Huo","submitted_at":"2011-11-15T21:00:02Z","abstract_excerpt":"Supersymmetric SO(10) Grand Unified Theories with Yukawa unification represent an appealing possibility for physics beyond the Standard Model. However Yukawa unification is made difficult by large threshold corrections to the bottom mass. Generally one is led to consider models where the sfermion masses are large in order to suppress these corrections. Here we present another possibility, in which the top and bottom GUT scale Yukawa couplings are equal to a component of the charged lepton Yukawa matrix at the GUT scale in a basis where this matrix is not diagonal. Physically, this weak eigenst"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.3639","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":""},"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":"1111.3639","created_at":"2026-05-18T01:59:32.775395+00:00"},{"alias_kind":"arxiv_version","alias_value":"1111.3639v1","created_at":"2026-05-18T01:59:32.775395+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.3639","created_at":"2026-05-18T01:59:32.775395+00:00"},{"alias_kind":"pith_short_12","alias_value":"SCQZUMYZXITT","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_16","alias_value":"SCQZUMYZXITTNTC7","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_8","alias_value":"SCQZUMYZ","created_at":"2026-05-18T12:26:41.206345+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/SCQZUMYZXITTNTC7NS2AWKC5AI","json":"https://pith.science/pith/SCQZUMYZXITTNTC7NS2AWKC5AI.json","graph_json":"https://pith.science/api/pith-number/SCQZUMYZXITTNTC7NS2AWKC5AI/graph.json","events_json":"https://pith.science/api/pith-number/SCQZUMYZXITTNTC7NS2AWKC5AI/events.json","paper":"https://pith.science/paper/SCQZUMYZ"},"agent_actions":{"view_html":"https://pith.science/pith/SCQZUMYZXITTNTC7NS2AWKC5AI","download_json":"https://pith.science/pith/SCQZUMYZXITTNTC7NS2AWKC5AI.json","view_paper":"https://pith.science/paper/SCQZUMYZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1111.3639&json=true","fetch_graph":"https://pith.science/api/pith-number/SCQZUMYZXITTNTC7NS2AWKC5AI/graph.json","fetch_events":"https://pith.science/api/pith-number/SCQZUMYZXITTNTC7NS2AWKC5AI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SCQZUMYZXITTNTC7NS2AWKC5AI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SCQZUMYZXITTNTC7NS2AWKC5AI/action/storage_attestation","attest_author":"https://pith.science/pith/SCQZUMYZXITTNTC7NS2AWKC5AI/action/author_attestation","sign_citation":"https://pith.science/pith/SCQZUMYZXITTNTC7NS2AWKC5AI/action/citation_signature","submit_replication":"https://pith.science/pith/SCQZUMYZXITTNTC7NS2AWKC5AI/action/replication_record"}},"created_at":"2026-05-18T01:59:32.775395+00:00","updated_at":"2026-05-18T01:59:32.775395+00:00"}