suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM2_i2.dat, 2:590|1.9e-09, 4:500|5.2e-10
suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM3_i2.dat, 2:863|2.1e-09, 4:849|4.3e-09
suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM5_i2.dat, 2:2338|4.8e-09, 4:1226|1.9e-09
suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM10_i2.dat, 2:5272|2.6e-09, 4:6162|4.4e-09
suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM20_i2.dat, 2:18590|2.9e-09, 4:16790|2.3e-09