{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:FJAFHBYHFWDQFIJAK5UMJ5QPXT","short_pith_number":"pith:FJAFHBYH","schema_version":"1.0","canonical_sha256":"2a405387072d8702a1205768c4f60fbcd97d6dd6d2a580c21e74e9c8d8b593c2","source":{"kind":"arxiv","id":"1102.5148","version":1},"attestation_state":"computed","paper":{"title":"Fermion Masses in SO(10) Models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Anjan S. Joshipura, Ketan M. Patel","submitted_at":"2011-02-25T03:50:20Z","abstract_excerpt":"We examine many SO(10) models for their viability or otherwise in explaining all the fermion masses and mixing angles. This study is carried out for both supersymmetric and non-supersymmetric models and with minimal ($10+\\bar{126}$) and non-minimal ($10+\\bar{126}+120$) Higgs content. Extensive numerical fits to fermion masses and mixing are carried out in each case assuming dominance of type-II or type-I seesaw mechanism. Required scale of the B-L breaking is identified in each case. In supersymmetric case, several sets of data at the GUT scale with or without inclusion of finite supersymmetri"},"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":"1102.5148","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-02-25T03:50:20Z","cross_cats_sorted":[],"title_canon_sha256":"735a556595c2328bfbd11ba6307162c5aec9c7dfe35f452d4257cb45e1553d75","abstract_canon_sha256":"e92327f50de64a7455b5f1dcfddd81e447ed8b7fdf886000604ccee5399b377b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:22:21.837336Z","signature_b64":"l9XHFsqBCtc+lNpp4KxDvAtPmpZNCqZ6N1HeZ3e8ljrr8XvdgI3tOZEdZBDCHrsJfjghqO6EKdEKW7ZpqQ4uBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2a405387072d8702a1205768c4f60fbcd97d6dd6d2a580c21e74e9c8d8b593c2","last_reissued_at":"2026-05-18T04:22:21.836837Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:22:21.836837Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fermion Masses in SO(10) Models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Anjan S. Joshipura, Ketan M. Patel","submitted_at":"2011-02-25T03:50:20Z","abstract_excerpt":"We examine many SO(10) models for their viability or otherwise in explaining all the fermion masses and mixing angles. This study is carried out for both supersymmetric and non-supersymmetric models and with minimal ($10+\\bar{126}$) and non-minimal ($10+\\bar{126}+120$) Higgs content. Extensive numerical fits to fermion masses and mixing are carried out in each case assuming dominance of type-II or type-I seesaw mechanism. Required scale of the B-L breaking is identified in each case. In supersymmetric case, several sets of data at the GUT scale with or without inclusion of finite supersymmetri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.5148","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":"1102.5148","created_at":"2026-05-18T04:22:21.836904+00:00"},{"alias_kind":"arxiv_version","alias_value":"1102.5148v1","created_at":"2026-05-18T04:22:21.836904+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.5148","created_at":"2026-05-18T04:22:21.836904+00:00"},{"alias_kind":"pith_short_12","alias_value":"FJAFHBYHFWDQ","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_16","alias_value":"FJAFHBYHFWDQFIJA","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_8","alias_value":"FJAFHBYH","created_at":"2026-05-18T12:26:28.662955+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.04021","citing_title":"Reality-constrained Minimal Yukawa Structure in SO(10) GUT","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06362","citing_title":"Towards Precision Neutrino Fits in GUTs: Relevance of One-Loop Finite Corrections","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FJAFHBYHFWDQFIJAK5UMJ5QPXT","json":"https://pith.science/pith/FJAFHBYHFWDQFIJAK5UMJ5QPXT.json","graph_json":"https://pith.science/api/pith-number/FJAFHBYHFWDQFIJAK5UMJ5QPXT/graph.json","events_json":"https://pith.science/api/pith-number/FJAFHBYHFWDQFIJAK5UMJ5QPXT/events.json","paper":"https://pith.science/paper/FJAFHBYH"},"agent_actions":{"view_html":"https://pith.science/pith/FJAFHBYHFWDQFIJAK5UMJ5QPXT","download_json":"https://pith.science/pith/FJAFHBYHFWDQFIJAK5UMJ5QPXT.json","view_paper":"https://pith.science/paper/FJAFHBYH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1102.5148&json=true","fetch_graph":"https://pith.science/api/pith-number/FJAFHBYHFWDQFIJAK5UMJ5QPXT/graph.json","fetch_events":"https://pith.science/api/pith-number/FJAFHBYHFWDQFIJAK5UMJ5QPXT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FJAFHBYHFWDQFIJAK5UMJ5QPXT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FJAFHBYHFWDQFIJAK5UMJ5QPXT/action/storage_attestation","attest_author":"https://pith.science/pith/FJAFHBYHFWDQFIJAK5UMJ5QPXT/action/author_attestation","sign_citation":"https://pith.science/pith/FJAFHBYHFWDQFIJAK5UMJ5QPXT/action/citation_signature","submit_replication":"https://pith.science/pith/FJAFHBYHFWDQFIJAK5UMJ5QPXT/action/replication_record"}},"created_at":"2026-05-18T04:22:21.836904+00:00","updated_at":"2026-05-18T04:22:21.836904+00:00"}