{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:QBK3PUKMUIZN4TFY7WTDCFYAER","short_pith_number":"pith:QBK3PUKM","schema_version":"1.0","canonical_sha256":"8055b7d14ca232de4cb8fda63117002442d9691bc8b1434c0d21d20115c7fb80","source":{"kind":"arxiv","id":"1811.07877","version":3},"attestation_state":"computed","paper":{"title":"Fermion Pair Production in SO(5) x U(1) Gauge-Higgs Unification Models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jongmin Yoon, Michael E. Peskin","submitted_at":"2018-11-19T18:51:46Z","abstract_excerpt":"We compute fermion pair production cross sections in $e^+e^-$ annihilation in models of electroweak symmetry breaking in warped 5-dimensional space. Our analysis is based on a framework with no elementary scalars, only gauge bosons and fermions in the bulk. We apply a novel Green's function method to obtain an analytic understanding of the new physics effects across the parameter space. We present results for $e^+e^-\\to b\\bar b$ and $e^+e^-\\to t\\bar t$. The predicted effects will be visible in precision measurements. Different models of $b$ quark mass generation can be distinguished by these m"},"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":"1811.07877","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-11-19T18:51:46Z","cross_cats_sorted":[],"title_canon_sha256":"7b03b2f11052b786096dbd56e4ea1fc9dfaa1af1497c5114dc2da873180ee0ce","abstract_canon_sha256":"471a1088f8d12af320c7dc55eb2ca6c9ad201f81a027e4898bd07a862cd04dc7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:56:40.790989Z","signature_b64":"Tjw81s8v6ixF+UiLMyNlWXxKjZqEwHN4eHRSX9g8VyG6bysKXsAdrdjqo9suRnWF/svME/aH49F3nxQeK5OWBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8055b7d14ca232de4cb8fda63117002442d9691bc8b1434c0d21d20115c7fb80","last_reissued_at":"2026-05-17T23:56:40.790391Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:56:40.790391Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fermion Pair Production in SO(5) x U(1) Gauge-Higgs Unification Models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jongmin Yoon, Michael E. Peskin","submitted_at":"2018-11-19T18:51:46Z","abstract_excerpt":"We compute fermion pair production cross sections in $e^+e^-$ annihilation in models of electroweak symmetry breaking in warped 5-dimensional space. Our analysis is based on a framework with no elementary scalars, only gauge bosons and fermions in the bulk. We apply a novel Green's function method to obtain an analytic understanding of the new physics effects across the parameter space. We present results for $e^+e^-\\to b\\bar b$ and $e^+e^-\\to t\\bar t$. The predicted effects will be visible in precision measurements. Different models of $b$ quark mass generation can be distinguished by these m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.07877","kind":"arxiv","version":3},"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":"1811.07877","created_at":"2026-05-17T23:56:40.790488+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.07877v3","created_at":"2026-05-17T23:56:40.790488+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.07877","created_at":"2026-05-17T23:56:40.790488+00:00"},{"alias_kind":"pith_short_12","alias_value":"QBK3PUKMUIZN","created_at":"2026-05-18T12:32:46.962924+00:00"},{"alias_kind":"pith_short_16","alias_value":"QBK3PUKMUIZN4TFY","created_at":"2026-05-18T12:32:46.962924+00:00"},{"alias_kind":"pith_short_8","alias_value":"QBK3PUKM","created_at":"2026-05-18T12:32:46.962924+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/QBK3PUKMUIZN4TFY7WTDCFYAER","json":"https://pith.science/pith/QBK3PUKMUIZN4TFY7WTDCFYAER.json","graph_json":"https://pith.science/api/pith-number/QBK3PUKMUIZN4TFY7WTDCFYAER/graph.json","events_json":"https://pith.science/api/pith-number/QBK3PUKMUIZN4TFY7WTDCFYAER/events.json","paper":"https://pith.science/paper/QBK3PUKM"},"agent_actions":{"view_html":"https://pith.science/pith/QBK3PUKMUIZN4TFY7WTDCFYAER","download_json":"https://pith.science/pith/QBK3PUKMUIZN4TFY7WTDCFYAER.json","view_paper":"https://pith.science/paper/QBK3PUKM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.07877&json=true","fetch_graph":"https://pith.science/api/pith-number/QBK3PUKMUIZN4TFY7WTDCFYAER/graph.json","fetch_events":"https://pith.science/api/pith-number/QBK3PUKMUIZN4TFY7WTDCFYAER/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QBK3PUKMUIZN4TFY7WTDCFYAER/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QBK3PUKMUIZN4TFY7WTDCFYAER/action/storage_attestation","attest_author":"https://pith.science/pith/QBK3PUKMUIZN4TFY7WTDCFYAER/action/author_attestation","sign_citation":"https://pith.science/pith/QBK3PUKMUIZN4TFY7WTDCFYAER/action/citation_signature","submit_replication":"https://pith.science/pith/QBK3PUKMUIZN4TFY7WTDCFYAER/action/replication_record"}},"created_at":"2026-05-17T23:56:40.790488+00:00","updated_at":"2026-05-17T23:56:40.790488+00:00"}