{"id":"W2081793557","doi":"10.1103/physreve.84.041803","title":"Dependence of the disorder-lamellar stability boundary of a melt of asymmetric wormlike<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>A</mml:mi><mml:mi>B</mml:mi></mml:mrow></mml:math>diblock copolymers on the chain rigidity","year":2011,"lang":"lv","type":"article","venue":"Physical Review E","topic":"Block Copolymer Self-Assembly","field":"Materials Science","cited_by":26,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Waterloo","funders":"Natural Sciences and Engineering Research Council of Canada","keywords":"Gaussian; Phase diagram; Phase boundary; Phase transition; Statistical physics; Thermodynamics; Lamellar structure; Chain (unit); Materials science; Phase (matter); Physics; Quantum mechanics","routes":{"ca_aff":true,"ca_fund":true,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":false},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"codex-gemma-dda1882f352a","candidate_categories":["metaepi_narrow","insufficient_payload"],"consensus_categories":[],"category_scores_codex":[0.002495283,0.0005697831,0.0005775975,0.0001373847,0.0006302187,0.0001946789,0.002417963,0.0004972967,0.007865279],"category_scores_gemma":[0.002496432,0.0006280577,0.001375481,0.00159355,0.001993979,0.0005209769,0.00157391,0.0008829443,0.0005211235],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00001769699,"about_ca_system_score_gemma":0.001185104,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.002197385,"about_ca_topic_score_gemma":0.0005106597,"domain_scores_codex":[0.9932545,0.0008433019,0.001546122,0.001078395,0.00217709,0.001100602],"domain_scores_gemma":[0.9925158,0.00199608,0.002258023,0.002672323,0.0001778863,0.0003798854],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"theoretical_or_conceptual","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.0004367603,0.001101245,0.00004220677,0.004661585,0.0004057387,0.000038847,0.001455332,0.0000251877,0.01638618,0.9687592,0.003003065,0.003684678],"study_design_scores_gemma":[0.0005011357,0.001036421,0.0003444299,0.00298406,0.001066917,0.00005216959,0.0004714796,0.01532053,0.9764635,0.0006572496,0.000531642,0.0005704712],"study_design_candidate":"bench_or_experimental","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9626811,0.01085971,0.0001405606,0.0005165976,0.001057038,0.00013569,0.0002607162,0.00005455019,0.02429401],"genre_scores_gemma":[0.9925098,0.005590516,0.0003396417,0.000645159,0.0003523193,0.000337192,0.00004121108,0.0001653648,0.00001880583],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.9681019,"threshold_uncertainty_score":0.9996171,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.02471591913014223,"score_gpt":0.2555340326056328,"score_spread":0.2308181134754906,"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."}}