{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:GLDC4LZUBMOOKCGEKQ3ITO73KD","short_pith_number":"pith:GLDC4LZU","schema_version":"1.0","canonical_sha256":"32c62e2f340b1ce508c4543689bbfb50c4b8f07f5a33750ef66725af8ca44f00","source":{"kind":"arxiv","id":"hep-ph/9802329","version":2},"attestation_state":"computed","paper":{"title":"Yukawa-coupling corrections to scalar quark decays","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jaume Guasch, Joan Sola, Wolfgang Hollik","submitted_at":"1998-02-16T13:54:09Z","abstract_excerpt":"Heavy squark decays into top and charginos or neutralinos could be an unexpected source of top quarks at hadron colliders. A detailed treatment of these processes is necessary for a reliable calculation of both the top quark production cross-section and the standard top quark branching ratio in the MSSM. Along this line we compute the electroweak corrections to the sbottom decays sbottom_a --> chargino_i top within the Yukawa coupling approximation. The calculation of these higher order contributions requires renormalization of both the bottom squark mixing angle and of tan(beta). This type of"},"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/9802329","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-02-16T13:54:09Z","cross_cats_sorted":[],"title_canon_sha256":"7a7dc16dd13e13fbac05a66fee5e71bb7a170ef9635c16713cbf1343a35748f2","abstract_canon_sha256":"77f80a77aad50b1c8fa648c1fb7e67e52ca760a6ba34bd4bd7c81e3cb52e92bc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:30:45.811623Z","signature_b64":"wZCt0C98w1QlcjZbuAXaXhx0SqulbqVIrirNDI5tBcHyxjH90eLuHUWyRUzUFJXQfpgRmvRzaJPcbFL9jNOkBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"32c62e2f340b1ce508c4543689bbfb50c4b8f07f5a33750ef66725af8ca44f00","last_reissued_at":"2026-05-18T04:30:45.811124Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:30:45.811124Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Yukawa-coupling corrections to scalar quark decays","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jaume Guasch, Joan Sola, Wolfgang Hollik","submitted_at":"1998-02-16T13:54:09Z","abstract_excerpt":"Heavy squark decays into top and charginos or neutralinos could be an unexpected source of top quarks at hadron colliders. A detailed treatment of these processes is necessary for a reliable calculation of both the top quark production cross-section and the standard top quark branching ratio in the MSSM. Along this line we compute the electroweak corrections to the sbottom decays sbottom_a --> chargino_i top within the Yukawa coupling approximation. The calculation of these higher order contributions requires renormalization of both the bottom squark mixing angle and of tan(beta). This type of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9802329","kind":"arxiv","version":2},"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/9802329","created_at":"2026-05-18T04:30:45.811204+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9802329v2","created_at":"2026-05-18T04:30:45.811204+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9802329","created_at":"2026-05-18T04:30:45.811204+00:00"},{"alias_kind":"pith_short_12","alias_value":"GLDC4LZUBMOO","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_16","alias_value":"GLDC4LZUBMOOKCGE","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_8","alias_value":"GLDC4LZU","created_at":"2026-05-18T12:25:49.038998+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/GLDC4LZUBMOOKCGEKQ3ITO73KD","json":"https://pith.science/pith/GLDC4LZUBMOOKCGEKQ3ITO73KD.json","graph_json":"https://pith.science/api/pith-number/GLDC4LZUBMOOKCGEKQ3ITO73KD/graph.json","events_json":"https://pith.science/api/pith-number/GLDC4LZUBMOOKCGEKQ3ITO73KD/events.json","paper":"https://pith.science/paper/GLDC4LZU"},"agent_actions":{"view_html":"https://pith.science/pith/GLDC4LZUBMOOKCGEKQ3ITO73KD","download_json":"https://pith.science/pith/GLDC4LZUBMOOKCGEKQ3ITO73KD.json","view_paper":"https://pith.science/paper/GLDC4LZU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9802329&json=true","fetch_graph":"https://pith.science/api/pith-number/GLDC4LZUBMOOKCGEKQ3ITO73KD/graph.json","fetch_events":"https://pith.science/api/pith-number/GLDC4LZUBMOOKCGEKQ3ITO73KD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GLDC4LZUBMOOKCGEKQ3ITO73KD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GLDC4LZUBMOOKCGEKQ3ITO73KD/action/storage_attestation","attest_author":"https://pith.science/pith/GLDC4LZUBMOOKCGEKQ3ITO73KD/action/author_attestation","sign_citation":"https://pith.science/pith/GLDC4LZUBMOOKCGEKQ3ITO73KD/action/citation_signature","submit_replication":"https://pith.science/pith/GLDC4LZUBMOOKCGEKQ3ITO73KD/action/replication_record"}},"created_at":"2026-05-18T04:30:45.811204+00:00","updated_at":"2026-05-18T04:30:45.811204+00:00"}