suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM2_i1.dat, 2:410|1.3e-09, 4:470|6.3e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM3_i1.dat, 2:744|1.5e-09, 4:863|4.5e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM5_i1.dat, 2:1386|1.0e-09, 4:1562|6.2e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM10_i1.dat, 2:3912|6.0e-09, 4:3722|5.2e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM20_i1.dat, 2:14102|5.1e-09, 4:13886|5.5e-09