suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM2_i100.dat, 95:3460|5.1e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM3_i100.dat, 95:6430|8.0e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM5_i100.dat, 95:11532|4.3e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM10_i100.dat, 95:38765|6.5e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM20_i100.dat, 95:132018|1.7e-09
suite = 'bbob', funcId = 18, DIM = 40, 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_f18/bbobexp_f18_DIM40_i100.dat, 95:221346|2.0e-09