suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM2_i2.dat, 2:2974|1.2e-10, 4:1467|5.7e-09
suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM3_i2.dat, 2:3917|5.0e-09, 4:14167|6.5e-10
suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM5_i2.dat, 2:902363|9.8e-01, 4:756275|8.9e-01
suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM10_i2.dat, 2:1405081|9.9e-01, 4:1447691|9.9e-01
suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM20_i2.dat, 2:3015035|5.0e+00, 4:2896031|7.0e+00