{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:YUMK3FTOGDIVKXMSFJNBAFCM5L","short_pith_number":"pith:YUMK3FTO","schema_version":"1.0","canonical_sha256":"c518ad966e30d1555d922a5a10144ceade3fcaf02b7b2f95b1dc29d91fabfe21","source":{"kind":"arxiv","id":"1611.08511","version":2},"attestation_state":"computed","paper":{"title":"A top-squark hunter's guide","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Howard Baer, Michael Savoy, Natsumi Nagata, Vernon Barger","submitted_at":"2016-11-25T16:35:31Z","abstract_excerpt":"In supersymmetric models with radiatively-driven naturalness and light higgsinos, the top squarks may lie in the 0.5- 3TeV range and thus only a fraction of natural parameter space is accessible to LHC searches. We outline the range of top squark and lightest SUSY particle masses preferred by electroweak naturalness in the standard parameter space plane. We note that the branching fraction for b-> s\\gamma decay favors top squarks much heavier than 500 GeV. Such a range of top-squark mass values is in contrast to previous expectations where m(stop)<500 GeV had been considered natural. In radiat"},"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":"1611.08511","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-25T16:35:31Z","cross_cats_sorted":[],"title_canon_sha256":"edceb971143863066e42d3df24fb3af37962b50d896f16acf728ff50b58497d3","abstract_canon_sha256":"f0ccf1112efaa60b1684e49e355d92b6b73bfcd04524f815696b5916e2a3cbd6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:48:16.138639Z","signature_b64":"RwRWCD6NFHRsdin+JtJY88MkNgCGDncyBWcaPMZY3Ws/iD3PPVCU0gnjZbNKvdDO2e6XUF3QET8YmYVeaQV8Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c518ad966e30d1555d922a5a10144ceade3fcaf02b7b2f95b1dc29d91fabfe21","last_reissued_at":"2026-05-18T00:48:16.137857Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:48:16.137857Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A top-squark hunter's guide","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Howard Baer, Michael Savoy, Natsumi Nagata, Vernon Barger","submitted_at":"2016-11-25T16:35:31Z","abstract_excerpt":"In supersymmetric models with radiatively-driven naturalness and light higgsinos, the top squarks may lie in the 0.5- 3TeV range and thus only a fraction of natural parameter space is accessible to LHC searches. We outline the range of top squark and lightest SUSY particle masses preferred by electroweak naturalness in the standard parameter space plane. We note that the branching fraction for b-> s\\gamma decay favors top squarks much heavier than 500 GeV. Such a range of top-squark mass values is in contrast to previous expectations where m(stop)<500 GeV had been considered natural. In radiat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.08511","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":"1611.08511","created_at":"2026-05-18T00:48:16.138006+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.08511v2","created_at":"2026-05-18T00:48:16.138006+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.08511","created_at":"2026-05-18T00:48:16.138006+00:00"},{"alias_kind":"pith_short_12","alias_value":"YUMK3FTOGDIV","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_16","alias_value":"YUMK3FTOGDIVKXMS","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_8","alias_value":"YUMK3FTO","created_at":"2026-05-18T12:30:53.716459+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/YUMK3FTOGDIVKXMSFJNBAFCM5L","json":"https://pith.science/pith/YUMK3FTOGDIVKXMSFJNBAFCM5L.json","graph_json":"https://pith.science/api/pith-number/YUMK3FTOGDIVKXMSFJNBAFCM5L/graph.json","events_json":"https://pith.science/api/pith-number/YUMK3FTOGDIVKXMSFJNBAFCM5L/events.json","paper":"https://pith.science/paper/YUMK3FTO"},"agent_actions":{"view_html":"https://pith.science/pith/YUMK3FTOGDIVKXMSFJNBAFCM5L","download_json":"https://pith.science/pith/YUMK3FTOGDIVKXMSFJNBAFCM5L.json","view_paper":"https://pith.science/paper/YUMK3FTO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.08511&json=true","fetch_graph":"https://pith.science/api/pith-number/YUMK3FTOGDIVKXMSFJNBAFCM5L/graph.json","fetch_events":"https://pith.science/api/pith-number/YUMK3FTOGDIVKXMSFJNBAFCM5L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YUMK3FTOGDIVKXMSFJNBAFCM5L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YUMK3FTOGDIVKXMSFJNBAFCM5L/action/storage_attestation","attest_author":"https://pith.science/pith/YUMK3FTOGDIVKXMSFJNBAFCM5L/action/author_attestation","sign_citation":"https://pith.science/pith/YUMK3FTOGDIVKXMSFJNBAFCM5L/action/citation_signature","submit_replication":"https://pith.science/pith/YUMK3FTOGDIVKXMSFJNBAFCM5L/action/replication_record"}},"created_at":"2026-05-18T00:48:16.138006+00:00","updated_at":"2026-05-18T00:48:16.138006+00:00"}