suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM2_i2.dat, 1:873|2.1e-11, 3:1564|2.0e-09, 5:260|3.0e-09
suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM3_i2.dat, 1:284211|1.8e-04, 3:2244|9.7e-11, 5:283749|3.8e-05
suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM5_i2.dat, 1:4108|2.7e-10, 3:4332|6.0e-10, 5:331531|2.2e-01
suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM10_i2.dat, 1:554561|2.0e+00, 3:576731|6.9e-01, 5:638271|5.1e+00
suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM20_i2.dat, 1:999071|2.0e+00, 3:1044899|2.6e+00, 5:1063763|5.1e+00