suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM2_i1.dat, 2:5405|2.1e-09, 4:1155|5.3e-09
suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM3_i1.dat, 2:25375|2.1e-10, 4:15364|7.9e-09
suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM5_i1.dat, 2:12901|2.5e-09, 4:40127|5.9e-10
suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM10_i1.dat, 2:752170|3.0e-10, 4:437159|1.1e-10
suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM20_i1.dat, 2:4001339|5.9e-02, 4:2152954|2.2e-11