{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:MSYTBL6OPE7W2DM66E4U2YJG34","short_pith_number":"pith:MSYTBL6O","schema_version":"1.0","canonical_sha256":"64b130afce793f6d0d9ef1394d6126df2848908a126f1eed35127fcea57ca8f9","source":{"kind":"arxiv","id":"1607.02050","version":2},"attestation_state":"computed","paper":{"title":"Scalar versus fermionic top partner interpretations of $t\\bar t + E_T^{\\rm miss}$ searches at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Hugo Prager, Luca Panizzi, Sabine Kraml, Ursula Laa","submitted_at":"2016-07-07T15:39:43Z","abstract_excerpt":"We assess how different ATLAS and CMS searches for supersymmetry in the $t\\bar t + E_T^{\\rm miss}$ final state at Run 1 of the LHC constrain scenarios with a fermionic top partner and a dark matter candidate. We find that the efficiencies of these searches in all-hadronic, 1-lepton and 2-lepton channels are quite similar for scalar and fermionic top partners. Therefore, in general, efficiency maps for stop-neutralino simplified models can also be applied to fermionic top-partner models, provided the narrow width approximation holds in the latter. Owing to the much higher production cross-secti"},"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":"1607.02050","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-07-07T15:39:43Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"c68e4565c55ecfc82fa4c4184466482452dce6401cf00404c3e3302178e5c9e6","abstract_canon_sha256":"06fba6b7142f7467970081de96f9ca788259ec1e98b69dc9bf89cb629895c624"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:56:45.836694Z","signature_b64":"pbH+5vEsV7wSjqWgFwQxDr8QVqc/Nl520Eta+o75VE0FRZcIsTpU60tZ7Fg6i84dzYW0FOvwkC+aIT46nYsoCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"64b130afce793f6d0d9ef1394d6126df2848908a126f1eed35127fcea57ca8f9","last_reissued_at":"2026-05-18T00:56:45.836064Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:56:45.836064Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scalar versus fermionic top partner interpretations of $t\\bar t + E_T^{\\rm miss}$ searches at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Hugo Prager, Luca Panizzi, Sabine Kraml, Ursula Laa","submitted_at":"2016-07-07T15:39:43Z","abstract_excerpt":"We assess how different ATLAS and CMS searches for supersymmetry in the $t\\bar t + E_T^{\\rm miss}$ final state at Run 1 of the LHC constrain scenarios with a fermionic top partner and a dark matter candidate. We find that the efficiencies of these searches in all-hadronic, 1-lepton and 2-lepton channels are quite similar for scalar and fermionic top partners. Therefore, in general, efficiency maps for stop-neutralino simplified models can also be applied to fermionic top-partner models, provided the narrow width approximation holds in the latter. Owing to the much higher production cross-secti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.02050","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":"1607.02050","created_at":"2026-05-18T00:56:45.836178+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.02050v2","created_at":"2026-05-18T00:56:45.836178+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.02050","created_at":"2026-05-18T00:56:45.836178+00:00"},{"alias_kind":"pith_short_12","alias_value":"MSYTBL6OPE7W","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_16","alias_value":"MSYTBL6OPE7W2DM6","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_8","alias_value":"MSYTBL6O","created_at":"2026-05-18T12:30:32.724797+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/MSYTBL6OPE7W2DM66E4U2YJG34","json":"https://pith.science/pith/MSYTBL6OPE7W2DM66E4U2YJG34.json","graph_json":"https://pith.science/api/pith-number/MSYTBL6OPE7W2DM66E4U2YJG34/graph.json","events_json":"https://pith.science/api/pith-number/MSYTBL6OPE7W2DM66E4U2YJG34/events.json","paper":"https://pith.science/paper/MSYTBL6O"},"agent_actions":{"view_html":"https://pith.science/pith/MSYTBL6OPE7W2DM66E4U2YJG34","download_json":"https://pith.science/pith/MSYTBL6OPE7W2DM66E4U2YJG34.json","view_paper":"https://pith.science/paper/MSYTBL6O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.02050&json=true","fetch_graph":"https://pith.science/api/pith-number/MSYTBL6OPE7W2DM66E4U2YJG34/graph.json","fetch_events":"https://pith.science/api/pith-number/MSYTBL6OPE7W2DM66E4U2YJG34/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MSYTBL6OPE7W2DM66E4U2YJG34/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MSYTBL6OPE7W2DM66E4U2YJG34/action/storage_attestation","attest_author":"https://pith.science/pith/MSYTBL6OPE7W2DM66E4U2YJG34/action/author_attestation","sign_citation":"https://pith.science/pith/MSYTBL6OPE7W2DM66E4U2YJG34/action/citation_signature","submit_replication":"https://pith.science/pith/MSYTBL6OPE7W2DM66E4U2YJG34/action/replication_record"}},"created_at":"2026-05-18T00:56:45.836178+00:00","updated_at":"2026-05-18T00:56:45.836178+00:00"}