suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM2_i1.dat, 2:674|3.1e-09, 4:440|2.0e-09
suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM3_i1.dat, 2:2074|9.1e-09, 4:898|3.1e-09
suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM5_i1.dat, 2:1602|5.8e-09, 4:1698|7.7e-09
suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM10_i1.dat, 2:8222|8.4e-09, 4:14022|9.5e-09
suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM20_i1.dat, 2:10346|9.1e-09, 4:19658|9.3e-09