suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM2_i2.dat, 1:380|9.0e-09, 3:470|2.8e-09, 5:368|3.6e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM3_i2.dat, 1:751|2.1e-09, 3:695|4.8e-09, 5:772|7.7e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM5_i2.dat, 1:1290|8.1e-09, 3:1402|3.1e-09, 5:1274|3.8e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM10_i2.dat, 1:3832|6.3e-09, 3:4162|3.1e-09, 5:3872|5.4e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM20_i2.dat, 1:13562|7.9e-09, 3:13574|6.3e-09, 5:13910|6.0e-09