suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM2_i1.dat, 1:254|6.1e-10, 3:284|1.2e-09, 5:254|2.2e-09
suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM3_i1.dat, 1:415|3.8e-09, 3:352|7.0e-09, 5:366|3.8e-09
suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM5_i1.dat, 1:762|4.4e-09, 3:682|6.2e-09, 5:738|5.0e-09
suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM10_i1.dat, 1:1272|7.0e-09, 3:1432|3.3e-09, 5:1242|7.8e-09
suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM20_i1.dat, 1:2750|3.5e-09, 3:2306|8.9e-09, 5:2438|5.3e-09