suite = 'bbob', funcId = 6, 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_f6/bbobexp_f6_DIM2_i2.dat, 1:566|3.0e-09, 3:680|5.8e-09, 5:446|4.2e-09
suite = 'bbob', funcId = 6, 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_f6/bbobexp_f6_DIM3_i2.dat, 1:912|6.0e-09, 3:828|6.3e-09, 5:751|8.4e-09
suite = 'bbob', funcId = 6, 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_f6/bbobexp_f6_DIM5_i2.dat, 1:1658|9.9e-09, 3:1634|6.2e-09, 5:1650|5.5e-09
suite = 'bbob', funcId = 6, 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_f6/bbobexp_f6_DIM10_i2.dat, 1:3462|9.2e-09, 3:4282|5.9e-09, 5:3702|9.5e-09
suite = 'bbob', funcId = 6, 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_f6/bbobexp_f6_DIM20_i2.dat, 1:9206|9.1e-09, 3:10790|7.8e-09, 5:10262|9.8e-09