suite = 'bbob', funcId = 5, DIM = 2, Precision = 1.000e-08, algId = 'a-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% a-CMA-ES: affine-invariant version of CMA-ES as benchmarked by A. Gissler in his BBOB-2023 paper
data_f5/bbobexp_f5_DIM2_i1.dat, 1:38|0.0e+00, 3:20|0.0e+00, 5:32|0.0e+00
suite = 'bbob', funcId = 5, DIM = 3, Precision = 1.000e-08, algId = 'a-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% a-CMA-ES: affine-invariant version of CMA-ES as benchmarked by A. Gissler in his BBOB-2023 paper
data_f5/bbobexp_f5_DIM3_i1.dat, 1:86|0.0e+00, 3:44|0.0e+00, 5:37|0.0e+00
suite = 'bbob', funcId = 5, DIM = 5, Precision = 1.000e-08, algId = 'a-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% a-CMA-ES: affine-invariant version of CMA-ES as benchmarked by A. Gissler in his BBOB-2023 paper
data_f5/bbobexp_f5_DIM5_i1.dat, 1:58|0.0e+00, 3:90|0.0e+00, 5:66|0.0e+00
suite = 'bbob', funcId = 5, DIM = 10, Precision = 1.000e-08, algId = 'a-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% a-CMA-ES: affine-invariant version of CMA-ES as benchmarked by A. Gissler in his BBOB-2023 paper
data_f5/bbobexp_f5_DIM10_i1.dat, 1:132|0.0e+00, 3:152|0.0e+00, 5:142|0.0e+00
suite = 'bbob', funcId = 5, DIM = 20, Precision = 1.000e-08, algId = 'a-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% a-CMA-ES: affine-invariant version of CMA-ES as benchmarked by A. Gissler in his BBOB-2023 paper
data_f5/bbobexp_f5_DIM20_i1.dat, 1:290|0.0e+00, 3:278|0.0e+00, 5:182|0.0e+00