suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM2_i2.dat, 2:974|2.9e-09, 4:3129|2.1e-09
suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM3_i2.dat, 2:5421|2.5e-09, 4:5722|3.1e-09
suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM5_i2.dat, 2:18788|3.4e-09, 4:3786|7.6e-09
suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM10_i2.dat, 2:2000800|1.5e-02, 4:120386|3.6e-09
suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM20_i2.dat, 2:102737|3.2e-09, 4:1086200|2.0e-09