{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:EYOO7KZ6JRTI2N6S4E6IVTQMJL","short_pith_number":"pith:EYOO7KZ6","schema_version":"1.0","canonical_sha256":"261cefab3e4c668d37d2e13c8ace0c4acce7a9a745824bbe340e16274a1af10a","source":{"kind":"arxiv","id":"hep-ph/9411218","version":1},"attestation_state":"computed","paper":{"title":"Fermion Masses in Superstring Theory","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"I. Antoniadis, T.R. Taylor","submitted_at":"1994-11-03T15:54:24Z","abstract_excerpt":"We give a model-independent discussion of fermion masses in four-dimensional heterotic superstring theories. We discuss the tree level contributions and quantum corrections, including one-loop threshold effects and masses generated as a result of non-perturbative supersymmetry breaking. We also point out that superstring models give rise to a generic $\\mu$-term in the effective low energy Lagrangian."},"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/9411218","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-11-03T15:54:24Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"38cf3f9e377eed19916772a089035dd1cf11822be092e4e3104e3cc68d6bee85","abstract_canon_sha256":"b1a156c236a0a43c141d566a0947e5d830b6cb219280c7f3ae48a8796761fb8e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:37:44.545103Z","signature_b64":"rvh5CdvVKyU80v0aW4Q2wBbbN2KGuj36xTsENUonEublKr34gH0nxWY5b64hXv1INTNGnpQi2Mz27MeMDvLsBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"261cefab3e4c668d37d2e13c8ace0c4acce7a9a745824bbe340e16274a1af10a","last_reissued_at":"2026-05-18T04:37:44.544643Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:37:44.544643Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fermion Masses in Superstring Theory","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"I. Antoniadis, T.R. Taylor","submitted_at":"1994-11-03T15:54:24Z","abstract_excerpt":"We give a model-independent discussion of fermion masses in four-dimensional heterotic superstring theories. We discuss the tree level contributions and quantum corrections, including one-loop threshold effects and masses generated as a result of non-perturbative supersymmetry breaking. We also point out that superstring models give rise to a generic $\\mu$-term in the effective low energy Lagrangian."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9411218","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":"hep-ph/9411218","created_at":"2026-05-18T04:37:44.544716+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9411218v1","created_at":"2026-05-18T04:37:44.544716+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9411218","created_at":"2026-05-18T04:37:44.544716+00:00"},{"alias_kind":"pith_short_12","alias_value":"EYOO7KZ6JRTI","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"EYOO7KZ6JRTI2N6S","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"EYOO7KZ6","created_at":"2026-05-18T12:25:47.102015+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/EYOO7KZ6JRTI2N6S4E6IVTQMJL","json":"https://pith.science/pith/EYOO7KZ6JRTI2N6S4E6IVTQMJL.json","graph_json":"https://pith.science/api/pith-number/EYOO7KZ6JRTI2N6S4E6IVTQMJL/graph.json","events_json":"https://pith.science/api/pith-number/EYOO7KZ6JRTI2N6S4E6IVTQMJL/events.json","paper":"https://pith.science/paper/EYOO7KZ6"},"agent_actions":{"view_html":"https://pith.science/pith/EYOO7KZ6JRTI2N6S4E6IVTQMJL","download_json":"https://pith.science/pith/EYOO7KZ6JRTI2N6S4E6IVTQMJL.json","view_paper":"https://pith.science/paper/EYOO7KZ6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9411218&json=true","fetch_graph":"https://pith.science/api/pith-number/EYOO7KZ6JRTI2N6S4E6IVTQMJL/graph.json","fetch_events":"https://pith.science/api/pith-number/EYOO7KZ6JRTI2N6S4E6IVTQMJL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EYOO7KZ6JRTI2N6S4E6IVTQMJL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EYOO7KZ6JRTI2N6S4E6IVTQMJL/action/storage_attestation","attest_author":"https://pith.science/pith/EYOO7KZ6JRTI2N6S4E6IVTQMJL/action/author_attestation","sign_citation":"https://pith.science/pith/EYOO7KZ6JRTI2N6S4E6IVTQMJL/action/citation_signature","submit_replication":"https://pith.science/pith/EYOO7KZ6JRTI2N6S4E6IVTQMJL/action/replication_record"}},"created_at":"2026-05-18T04:37:44.544716+00:00","updated_at":"2026-05-18T04:37:44.544716+00:00"}