{"id":"W2024496644","doi":"10.1142/s0217984911026024","title":"MACROSCOPIC AHARONOV–BOHM EFFECT AT L-BAND MICROWAVE FREQUENCIES","year":2011,"lang":"en","type":"article","venue":"Modern Physics Letters B","topic":"Quantum and electron transport phenomena","field":"Physics and Astronomy","cited_by":4,"is_retracted":false,"has_abstract":true,"ca_institutions":"McMaster University","funders":"","keywords":"Physics; Microwave; Gauge (firearms); Vector potential; Lorenz gauge condition; Range (aeronautics); Extremely high frequency; Computational physics; Waveguide; Mode (computer interface); Wave vector; Frequency band; Quantum electrodynamics; Optics; Acoustics; Gauge theory; Telecommunications; Quantum mechanics; Hamiltonian lattice gauge theory; Magnetic field; Computer science; Bandwidth (computing); Gauge anomaly","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":"codex-gemma-dda1882f352a","candidate_categories":["metaepi_narrow"],"consensus_categories":[],"category_scores_codex":[0.00008005118,0.0003436821,0.0003335814,0.0000328028,0.0002166491,0.00003670662,0.0002621429,0.00004088783,0.0003976139],"category_scores_gemma":[3.224248e-7,0.0003220065,0.0002071215,0.0001076162,0.0001358636,0.0002085354,0.00003374243,0.0002501375,0.0002968087],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.00006811547,"about_ca_system_score_gemma":0.000023197,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0002737694,"about_ca_topic_score_gemma":0.000007769741,"domain_scores_codex":[0.9984964,0.00004486188,0.0002255872,0.0004304579,0.0001721477,0.0006306014],"domain_scores_gemma":[0.999323,0.00003012431,0.0001030242,0.0004087147,0.0000219071,0.000113286],"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":[0.00006703519,0.0001580123,0.08549154,0.00004605297,0.0002253744,0.000008243576,0.003762838,0.00004051504,0.8967151,0.004995164,0.001555527,0.006934612],"study_design_scores_gemma":[0.001136304,0.0001413497,0.006356414,0.00003047016,0.0001173275,0.000001177082,0.000030424,0.0001648449,0.9575538,0.0332789,0.0005427966,0.0006461932],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9323118,0.00008162146,0.0554888,0.00008899967,0.000153329,0.0002296472,0.00004520686,0.00007042543,0.01153019],"genre_scores_gemma":[0.9983081,0.000001655943,0.000244064,0.0004750247,0.0003216083,0.00005880435,0.0001016518,0.00005692961,0.0004321933],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.07913513,"threshold_uncertainty_score":0.9999232,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.0123954969976335,"score_gpt":0.2012453448355574,"score_spread":0.1888498478379239,"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."}}