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_i2.dat, 2:254|2.2e-09, 4:230|1.4e-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_i2.dat, 2:429|5.2e-09, 4:303|4.1e-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_i2.dat, 2:706|9.3e-10, 4:650|9.9e-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_i2.dat, 2:1332|2.8e-09, 4:1412|5.3e-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_i2.dat, 2:2462|6.6e-09, 4:2426|7.7e-09