suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM2_i94.dat, 94:470|6.9e-09
suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM3_i94.dat, 94:758|1.1e-09
suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM5_i94.dat, 94:1242|9.8e-09
suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM10_i94.dat, 94:2862|5.9e-09
suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM20_i94.dat, 94:7106|5.4e-09
suite = 'bbob', funcId = 11, DIM = 40, 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_f11/bbobexp_f11_DIM40_i94.dat, 94:20147|6.0e-09