suite = 'bbob', funcId = 10, 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_f10/bbobexp_f10_DIM2_i1.dat, 2:344|5.5e-09, 4:512|5.7e-09
suite = 'bbob', funcId = 10, 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_f10/bbobexp_f10_DIM3_i1.dat, 2:688|1.3e-09, 4:926|5.4e-09
suite = 'bbob', funcId = 10, 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_f10/bbobexp_f10_DIM5_i1.dat, 2:1370|6.0e-09, 4:1410|5.3e-09
suite = 'bbob', funcId = 10, 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_f10/bbobexp_f10_DIM10_i1.dat, 2:4082|3.1e-09, 4:4162|6.0e-09
suite = 'bbob', funcId = 10, 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_f10/bbobexp_f10_DIM20_i1.dat, 2:13670|5.9e-09, 4:14474|5.7e-09