{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:PIZYKV26KAXA2CVSCFX3YFNA3D","short_pith_number":"pith:PIZYKV26","schema_version":"1.0","canonical_sha256":"7a3385575e502e0d0ab2116fbc15a0d8ec9fff01b2aaaa560086b3a08c24c089","source":{"kind":"arxiv","id":"2108.08080","version":1},"attestation_state":"computed","paper":{"title":"Nucleon decay in a minimal non-SUSY GUT with predicted quark-lepton Yukawa ratios","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kevin Hinze, Stefan Antusch","submitted_at":"2021-08-18T10:21:31Z","abstract_excerpt":"We investigate the predictions for various nucleon decay rates and their ratios in non-supersymmetric SU(5) Grand Unified Theories (GUTs) where the masses of the third and second family down-type quarks and charged leptons each stem dominantly from single GUT operators. Extending the Georgi-Glashow SU(5) model by a 45-dimensional GUT-Higgs representation, the gauge couplings can meet at the high scale $M_\\mathrm{GUT}$ and the GUT scale predictions $y_\\tau/y_b = 3/2$ and $y_\\mu/y_s = 9/2$ can emerge within single operator dominance. Explaining the observed neutrino masses via the type I seesaw "},"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":"2108.08080","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-08-18T10:21:31Z","cross_cats_sorted":[],"title_canon_sha256":"cd37102f63267c048e5e0cf8cfde5b700ab19454544ca26b3984501e4d069997","abstract_canon_sha256":"ccbd333db4f9d749b6757a8d3af3274d540478dd2e9e77e6f4e840c1e6baaa66"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:07:24.234912Z","signature_b64":"PZvpaTxt3JvcY7LINfLWpchMjLbWSPK5e7F8YKqvMGU8Lvpn9UdbpchOnAZO9Ch90WIETBWVeh1Eq4mG/hhfDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7a3385575e502e0d0ab2116fbc15a0d8ec9fff01b2aaaa560086b3a08c24c089","last_reissued_at":"2026-07-05T04:07:24.234399Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:07:24.234399Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nucleon decay in a minimal non-SUSY GUT with predicted quark-lepton Yukawa ratios","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kevin Hinze, Stefan Antusch","submitted_at":"2021-08-18T10:21:31Z","abstract_excerpt":"We investigate the predictions for various nucleon decay rates and their ratios in non-supersymmetric SU(5) Grand Unified Theories (GUTs) where the masses of the third and second family down-type quarks and charged leptons each stem dominantly from single GUT operators. Extending the Georgi-Glashow SU(5) model by a 45-dimensional GUT-Higgs representation, the gauge couplings can meet at the high scale $M_\\mathrm{GUT}$ and the GUT scale predictions $y_\\tau/y_b = 3/2$ and $y_\\mu/y_s = 9/2$ can emerge within single operator dominance. Explaining the observed neutrino masses via the type I seesaw "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2108.08080","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/2108.08080/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":"2108.08080","created_at":"2026-07-05T04:07:24.234458+00:00"},{"alias_kind":"arxiv_version","alias_value":"2108.08080v1","created_at":"2026-07-05T04:07:24.234458+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2108.08080","created_at":"2026-07-05T04:07:24.234458+00:00"},{"alias_kind":"pith_short_12","alias_value":"PIZYKV26KAXA","created_at":"2026-07-05T04:07:24.234458+00:00"},{"alias_kind":"pith_short_16","alias_value":"PIZYKV26KAXA2CVS","created_at":"2026-07-05T04:07:24.234458+00:00"},{"alias_kind":"pith_short_8","alias_value":"PIZYKV26","created_at":"2026-07-05T04:07:24.234458+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.16022","citing_title":"Non-Renormalizable SU(5) GUTs: Leptoquark-Induced Neutrino Masses","ref_index":63,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PIZYKV26KAXA2CVSCFX3YFNA3D","json":"https://pith.science/pith/PIZYKV26KAXA2CVSCFX3YFNA3D.json","graph_json":"https://pith.science/api/pith-number/PIZYKV26KAXA2CVSCFX3YFNA3D/graph.json","events_json":"https://pith.science/api/pith-number/PIZYKV26KAXA2CVSCFX3YFNA3D/events.json","paper":"https://pith.science/paper/PIZYKV26"},"agent_actions":{"view_html":"https://pith.science/pith/PIZYKV26KAXA2CVSCFX3YFNA3D","download_json":"https://pith.science/pith/PIZYKV26KAXA2CVSCFX3YFNA3D.json","view_paper":"https://pith.science/paper/PIZYKV26","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2108.08080&json=true","fetch_graph":"https://pith.science/api/pith-number/PIZYKV26KAXA2CVSCFX3YFNA3D/graph.json","fetch_events":"https://pith.science/api/pith-number/PIZYKV26KAXA2CVSCFX3YFNA3D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PIZYKV26KAXA2CVSCFX3YFNA3D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PIZYKV26KAXA2CVSCFX3YFNA3D/action/storage_attestation","attest_author":"https://pith.science/pith/PIZYKV26KAXA2CVSCFX3YFNA3D/action/author_attestation","sign_citation":"https://pith.science/pith/PIZYKV26KAXA2CVSCFX3YFNA3D/action/citation_signature","submit_replication":"https://pith.science/pith/PIZYKV26KAXA2CVSCFX3YFNA3D/action/replication_record"}},"created_at":"2026-07-05T04:07:24.234458+00:00","updated_at":"2026-07-05T04:07:24.234458+00:00"}