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_i2.dat, 1:1665|2.4e-09, 3:1635|5.1e-09, 5:1713|2.7e-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_i2.dat, 1:2754|8.3e-10, 3:6521|7.7e-09, 5:3069|1.5e-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_i2.dat, 1:5267|5.6e-09, 3:10444|8.4e-09, 5:6315|5.0e-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_i2.dat, 1:20874|3.2e-09, 3:38865|2.6e-09, 5:38955|3.9e-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_i2.dat, 1:125382|1.9e-09, 3:126258|1.3e-09, 5:125106|2.3e-09