suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM2_i1.dat, 1:3303|3.8e-09, 3:446|3.8e-10, 5:12360|6.5e-09
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM3_i1.dat, 1:14271|1.5e-09, 3:18709|3.1e-10, 5:42692|5.2e-09
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM5_i1.dat, 1:70054|5.1e-10, 3:163648|1.5e-10, 5:84062|8.4e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM10_i1.dat, 1:657589|1.5e-10, 3:876049|3.2e-10, 5:599429|3.9e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM20_i1.dat, 1:1599381|1.2e-10, 3:2855650|5.5e-11, 5:2761390|1.5e-10