suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM2_i2.dat, 2:3155|1.3e-15, 4:242|1.1e-09
suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM3_i2.dat, 2:268|2.8e-09, 4:275|1.5e-09
suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM5_i2.dat, 2:4244|1.8e-10, 4:13982|7.3e-11
suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM10_i2.dat, 2:74108|2.1e-12, 4:26266|4.7e-12
suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM20_i2.dat, 2:1006715|2.0e+00, 4:45966|1.1e-11