suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM2_i1.dat, 2:374|8.9e-09, 4:386|6.4e-09
suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM3_i1.dat, 2:618|5.2e-09, 4:751|8.3e-09
suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM5_i1.dat, 2:1218|8.2e-09, 4:1314|5.9e-09
suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM10_i1.dat, 2:3942|7.8e-09, 4:4002|8.5e-09
suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM20_i1.dat, 2:14030|9.7e-09, 4:14282|9.7e-09