suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM2_i2.dat, 2:590|5.8e-10, 4:434|7.5e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM3_i2.dat, 2:1052|9.2e-09, 4:1192|7.2e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM5_i2.dat, 2:2426|9.3e-09, 4:2730|9.7e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM10_i2.dat, 2:9702|1.0e-08, 4:15123|4.7e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM20_i2.dat, 2:127398|1.8e-09, 4:37647|8.0e-09