{"id":"W2093749273","doi":"10.1140/epje/i2011-11090-y","title":"Temperature behavior of the Kohlrausch exponent for a series of vinylic polymers modelled by an all-atomistic approach","year":2011,"lang":"en","type":"article","venue":"The European Physical Journal E","topic":"Material Dynamics and Properties","field":"Materials Science","cited_by":13,"is_retracted":false,"has_abstract":false,"ca_institutions":"Université de Sherbrooke","funders":"","keywords":"Exponent; Stretched exponential function; Exponential function; Relaxation (psychology); Polymer; Glass transition; Thermodynamics; Materials science; Phenomenological model; Series (stratigraphy); Statistical physics; Plateau (mathematics); Function (biology); Polymer chemistry; Physics; Condensed matter physics; Mathematics; Mathematical analysis; Composite material","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":[0.0003798726,0.0005529523,0.0005375192,0.0008073116,0.0005233383,0.0005389015,0.0006869665,0.0008162693,0.002390761],"category_scores_gemma":[0.001594789,0.0002780161,0.0005199755,0.0005153664,0.0008330378,0.0008766953,0.0003387887,0.0009388761,0.0001864063],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0006347782,"about_ca_system_score_gemma":0.0004751572,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.003873598,"about_ca_topic_score_gemma":0.002926205,"domain_scores_codex":[0.9999138,0.00002054951,0.000004970075,0.00001356013,0.00001791082,0.00002923371],"domain_scores_gemma":[0.9992022,0.0004340774,0.0001154474,0.00006838782,0.00009816462,0.0000818058],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.000297052,0.0001054284,0.002211595,0.0002421697,0.0000565403,0.0003349447,0.0002660455,0.9415368,0.02394617,0.02757259,0.0007461071,0.002684613],"study_design_scores_gemma":[0.00001735404,0.00006662705,0.001008356,0.00002110884,0.00001611574,0.00002283867,0.00003438886,0.9917042,0.003117513,0.003722691,0.0002456887,0.00002312033],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9898794,0.0006023153,0.004173147,0.0001688756,0.00005318073,0.00001699651,0.0001569819,0.00009470215,0.004854416],"genre_scores_gemma":[0.9981988,0.0001471517,0.0008029136,0.00001479442,0.000007489974,0.00001204996,0.00008485735,0.00003307392,0.0006988342],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.003873598,"threshold_uncertainty_score":0.00799793,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.03602327245281927,"score_gpt":0.2288611338177774,"score_spread":0.1928378613649581,"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."}}