suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM2_i2.dat, 2:548|3.0e-09, 4:308|3.7e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM3_i2.dat, 2:2411|2.7e-09, 4:23896|1.0e-09
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM5_i2.dat, 2:188704|8.8e-10, 4:84615|3.4e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM10_i2.dat, 2:701089|7.8e-11, 4:549859|1.9e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM20_i2.dat, 2:2922262|1.2e-10, 4:2525818|5.1e-11