{"id":"W2102900278","doi":"10.1103/physrevlett.104.251801","title":"Search for Pair Production of Supersymmetric Top Quarks in Dilepton Events from<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>p</mml:mi><mml:mover accent=\"true\"><mml:mi>p</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math>Collisions at<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo>=</mml:mo><mml:mn>1.96</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>TeV</mml:mi></mml:math>","year":2010,"lang":"lv","type":"article","venue":"Physical Review Letters","topic":"Particle physics theoretical and experimental studies","field":"Physics and Astronomy","cited_by":34,"is_retracted":false,"has_abstract":true,"ca_institutions":"McGill University; Institute of Particle Physics; Simon Fraser University; University of Toronto; TRIUMF","funders":"Science and Technology Facilities Council","keywords":"Neutralino; Chargino; Particle physics; Physics; Production (economics); Lepton; Supersymmetry; Branching fraction; Neutrino; Quark; Top quark; Combinatorics; Nuclear physics; Mathematics","routes":{"ca_aff":true,"ca_fund":false,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":false},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.0006352481,0.001477161,0.001149256,0.001846717,0.001204441,0.0018162,0.001406789,0.001219056,0.01901532],"category_scores_gemma":[0.0006276871,0.0007956905,0.001432109,0.002274598,0.0002870812,0.0005721663,0.001075921,0.0006877437,0.002892106],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0008594131,"about_ca_system_score_gemma":0.0005585105,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.003971429,"about_ca_topic_score_gemma":0.006445418,"domain_scores_codex":[0.9993713,0.000109957,0.00002927353,0.000164585,0.0001256107,0.0001992522],"domain_scores_gemma":[0.9994003,0.0002264701,0.0001248612,0.00004368313,0.0000616895,0.0001429622],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.0196391,0.001931093,0.3056755,0.001470922,0.002541493,0.0269106,0.002204931,0.03075598,0.4678277,0.0381877,0.04077616,0.06207877],"study_design_scores_gemma":[0.002563167,0.00270582,0.2288091,0.0001121309,0.00180855,0.006534784,0.001708238,0.21677,0.5069836,0.01723404,0.01425989,0.0005106819],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9518015,0.0003022549,0.01016286,0.0004154026,0.00004780123,0.0001168935,0.009260747,0.001614516,0.02627808],"genre_scores_gemma":[0.9789179,0.0001069877,0.005936488,0.0001628859,0.00002255349,0.00004479222,0.008618873,0.0002226801,0.005966763],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.01901532,"threshold_uncertainty_score":0.06361258,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01874866273139422,"score_gpt":0.2685262722771225,"score_spread":0.2497776095457283,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). Scores rank; they never assert a category."}}