suite = 'bbob', funcId = 8, 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_f8/bbobexp_f8_DIM2_i2.dat, 1:404|8.2e-09, 3:470|2.8e-09, 5:374|4.8e-10
suite = 'bbob', funcId = 8, 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_f8/bbobexp_f8_DIM3_i2.dat, 1:618|2.4e-09, 3:849|4.2e-09, 5:681|9.9e-10
suite = 'bbob', funcId = 8, 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_f8/bbobexp_f8_DIM5_i2.dat, 1:1802|3.6e-09, 3:1906|5.7e-09, 5:1770|5.2e-09
suite = 'bbob', funcId = 8, 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_f8/bbobexp_f8_DIM10_i2.dat, 1:5492|6.3e-09, 3:5292|7.9e-09, 5:5122|5.2e-09
suite = 'bbob', funcId = 8, 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_f8/bbobexp_f8_DIM20_i2.dat, 1:17570|5.5e-09, 3:17378|5.7e-09, 5:17150|7.3e-09