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_i1.dat, 1:566|1.1e-09, 3:314|6.4e-09, 5:398|7.2e-09
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_i1.dat, 1:786|3.3e-09, 3:779|2.6e-09, 5:716|2.4e-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_i1.dat, 1:1666|3.9e-09, 3:1450|6.0e-09, 5:2266|2.0e-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_i1.dat, 1:5032|3.3e-09, 3:10123|2.2e-09, 5:5212|5.7e-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_i1.dat, 1:14906|5.0e-09, 3:17714|5.2e-09, 5:15446|6.5e-09