{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:FP4K6I5Q4A3E5BQKANET6ITCLG","short_pith_number":"pith:FP4K6I5Q","schema_version":"1.0","canonical_sha256":"2bf8af23b0e0364e860a03493f226259a48c42e28e77bc706faa1e4446e07509","source":{"kind":"arxiv","id":"hep-ph/9906233","version":3},"attestation_state":"computed","paper":{"title":"Trilepton Signal for Supersymmetry at the Fermilab Tevatron Revisited","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Frank Paige, Howard Baer, Manuel Drees, Pamela Quintana, Xerxes Tata","submitted_at":"1999-06-03T14:15:49Z","abstract_excerpt":"Within a wide class of models, the LEP2 lower limit of 95 GeV on the chargino mass implies gluinos are heavier than $\\sim$300 GeV. In this case electroweak $\\tw_1\\twb_1$ and $\\tw_1\\tz_2$ production are the dominant SUSY processes at the Tevatron, and the extensively examined isolated trilepton signal from $\\tw_1\\tz_2$ production assumes an even greater importance. We update our previous calculations of the SUSY reach of luminosity upgrades of the Fermilab Tevatron in this channel incorporating ({\\it i}) decay matrix elements in the computation of the momenta of leptons from chargino and neutra"},"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/9906233","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1999-06-03T14:15:49Z","cross_cats_sorted":[],"title_canon_sha256":"8112c66bc40693c73de7cba7ebf8d8258e3929d0350f65b33a3a47e852e7773a","abstract_canon_sha256":"424bf576f7a9c0dd4b8fd7978a8672b851734f8fca4a097a39a3ec4712c525c6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:05.713667Z","signature_b64":"KmqSflYe6sAKozc3BBvpSZC+rPmBqfQbGgMXZ6bNxnG3lU1r3d8AM98EG4vvoynXvzJj/rjCBQ/684PZ3UQaAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2bf8af23b0e0364e860a03493f226259a48c42e28e77bc706faa1e4446e07509","last_reissued_at":"2026-05-18T01:06:05.713045Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:05.713045Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Trilepton Signal for Supersymmetry at the Fermilab Tevatron Revisited","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Frank Paige, Howard Baer, Manuel Drees, Pamela Quintana, Xerxes Tata","submitted_at":"1999-06-03T14:15:49Z","abstract_excerpt":"Within a wide class of models, the LEP2 lower limit of 95 GeV on the chargino mass implies gluinos are heavier than $\\sim$300 GeV. In this case electroweak $\\tw_1\\twb_1$ and $\\tw_1\\tz_2$ production are the dominant SUSY processes at the Tevatron, and the extensively examined isolated trilepton signal from $\\tw_1\\tz_2$ production assumes an even greater importance. We update our previous calculations of the SUSY reach of luminosity upgrades of the Fermilab Tevatron in this channel incorporating ({\\it i}) decay matrix elements in the computation of the momenta of leptons from chargino and neutra"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9906233","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":"hep-ph/9906233","created_at":"2026-05-18T01:06:05.713147+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9906233v3","created_at":"2026-05-18T01:06:05.713147+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9906233","created_at":"2026-05-18T01:06:05.713147+00:00"},{"alias_kind":"pith_short_12","alias_value":"FP4K6I5Q4A3E","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"FP4K6I5Q4A3E5BQK","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"FP4K6I5Q","created_at":"2026-05-18T12:25:49.631198+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/FP4K6I5Q4A3E5BQKANET6ITCLG","json":"https://pith.science/pith/FP4K6I5Q4A3E5BQKANET6ITCLG.json","graph_json":"https://pith.science/api/pith-number/FP4K6I5Q4A3E5BQKANET6ITCLG/graph.json","events_json":"https://pith.science/api/pith-number/FP4K6I5Q4A3E5BQKANET6ITCLG/events.json","paper":"https://pith.science/paper/FP4K6I5Q"},"agent_actions":{"view_html":"https://pith.science/pith/FP4K6I5Q4A3E5BQKANET6ITCLG","download_json":"https://pith.science/pith/FP4K6I5Q4A3E5BQKANET6ITCLG.json","view_paper":"https://pith.science/paper/FP4K6I5Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9906233&json=true","fetch_graph":"https://pith.science/api/pith-number/FP4K6I5Q4A3E5BQKANET6ITCLG/graph.json","fetch_events":"https://pith.science/api/pith-number/FP4K6I5Q4A3E5BQKANET6ITCLG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FP4K6I5Q4A3E5BQKANET6ITCLG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FP4K6I5Q4A3E5BQKANET6ITCLG/action/storage_attestation","attest_author":"https://pith.science/pith/FP4K6I5Q4A3E5BQKANET6ITCLG/action/author_attestation","sign_citation":"https://pith.science/pith/FP4K6I5Q4A3E5BQKANET6ITCLG/action/citation_signature","submit_replication":"https://pith.science/pith/FP4K6I5Q4A3E5BQKANET6ITCLG/action/replication_record"}},"created_at":"2026-05-18T01:06:05.713147+00:00","updated_at":"2026-05-18T01:06:05.713147+00:00"}