suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM2_i1.dat, 2:3430|7.0e-09, 4:1593|6.9e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM3_i1.dat, 2:6045|4.1e-09, 4:5583|3.7e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM5_i1.dat, 2:10708|4.3e-09, 4:11188|6.2e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM10_i1.dat, 2:41275|1.8e-09, 4:37405|2.8e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM20_i1.dat, 2:135486|1.9e-09, 4:127326|2.9e-09