suite = 'bbob', funcId = 4, DIM = 2, Precision = 1.000e-08, algId = 'COBYLA-scipy-2019', coco_version = '2.2.2', logger = 'bbob', data_format = 'bbob-new2'
% COBYLA-scipy-2019: COBYLA method from SciPy v1.2.1 as submitted by Varelas and Dahito to BBOB-2019
data_f4/bbobexp_f4_DIM2_i5.dat, 2:200020|2.0e-07, 8:200014|6.2e-08, 14:200024|8.5e-07
suite = 'bbob', funcId = 4, DIM = 3, Precision = 1.000e-08, algId = 'COBYLA-scipy-2019', coco_version = '2.2.2', logger = 'bbob', data_format = 'bbob-new2'
% COBYLA-scipy-2019: COBYLA method from SciPy v1.2.1 as submitted by Varelas and Dahito to BBOB-2019
data_f4/bbobexp_f4_DIM3_i5.dat, 2:300257|1.1e-03, 8:300060|1.2e-04, 14:300025|5.2e-03
suite = 'bbob', funcId = 4, DIM = 5, Precision = 1.000e-08, algId = 'COBYLA-scipy-2019', coco_version = '2.2.2', logger = 'bbob', data_format = 'bbob-new2'
% COBYLA-scipy-2019: COBYLA method from SciPy v1.2.1 as submitted by Varelas and Dahito to BBOB-2019
data_f4/bbobexp_f4_DIM5_i5.dat, 2:500500|2.0e+00, 8:500018|2.0e+00, 14:502573|2.0e+00
suite = 'bbob', funcId = 4, DIM = 10, Precision = 1.000e-08, algId = 'COBYLA-scipy-2019', coco_version = '2.2.2', logger = 'bbob', data_format = 'bbob-new2'
% COBYLA-scipy-2019: COBYLA method from SciPy v1.2.1 as submitted by Varelas and Dahito to BBOB-2019
data_f4/bbobexp_f4_DIM10_i5.dat, 2:1000628|2.7e+01, 8:1001414|2.3e+01, 14:1000766|9.0e+00
suite = 'bbob', funcId = 4, DIM = 20, Precision = 1.000e-08, algId = 'COBYLA-scipy-2019', coco_version = '2.2.2', logger = 'bbob', data_format = 'bbob-new2'
% COBYLA-scipy-2019: COBYLA method from SciPy v1.2.1 as submitted by Varelas and Dahito to BBOB-2019
data_f4/bbobexp_f4_DIM20_i5.dat, 2:2008470|1.2e+02, 8:2008119|1.4e+02, 14:2000612|1.1e+02
suite = 'bbob', funcId = 4, DIM = 40, Precision = 1.000e-08, algId = 'COBYLA-scipy-2019', coco_version = '2.2.2', logger = 'bbob', data_format = 'bbob-new2'
% COBYLA-scipy-2019: COBYLA method from SciPy v1.2.1 as submitted by Varelas and Dahito to BBOB-2019
data_f4/bbobexp_f4_DIM40_i5.dat, 2:4003011|4.4e+02, 8:4001429|4.5e+02, 14:4001992|3.8e+02