suite = 'bbob', funcId = 17, 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_f17/bbobexp_f17_DIM2_i1.dat, 1:1569|1.2e-09, 3:1845|1.5e-09, 5:1497|5.2e-09
suite = 'bbob', funcId = 17, 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_f17/bbobexp_f17_DIM3_i1.dat, 1:2544|7.8e-09, 3:1122|2.0e-09, 5:4589|5.6e-09
suite = 'bbob', funcId = 17, 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_f17/bbobexp_f17_DIM5_i1.dat, 1:10148|3.6e-09, 3:5675|7.9e-09, 5:9564|3.9e-09
suite = 'bbob', funcId = 17, 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_f17/bbobexp_f17_DIM10_i1.dat, 1:37305|2.5e-09, 3:20424|3.9e-09, 5:20464|3.7e-09
suite = 'bbob', funcId = 17, 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_f17/bbobexp_f17_DIM20_i1.dat, 1:121110|1.7e-09, 3:62525|2.0e-09, 5:63185|2.8e-09