suite = 'bbob', funcId = 17, DIM = 2, Precision = 1.000e-08, algId = 's-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% s-CMA-ES: CMA-ES without cumulation for the step size as benchmarked by A. Gissler in his BBOB-2023 paper
data_f17/bbobexp_f17_DIM2_i1.dat, 1:1713|4.1e-09, 3:1455|5.6e-09, 5:1563|3.5e-09
suite = 'bbob', funcId = 17, DIM = 3, Precision = 1.000e-08, algId = 's-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% s-CMA-ES: CMA-ES without cumulation for the step size as benchmarked by A. Gissler in his BBOB-2023 paper
data_f17/bbobexp_f17_DIM3_i1.dat, 1:5247|4.7e-09, 3:3377|3.5e-09, 5:5520|3.5e-09
suite = 'bbob', funcId = 17, DIM = 5, Precision = 1.000e-08, algId = 's-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% s-CMA-ES: CMA-ES without cumulation for the step size as benchmarked by A. Gissler in his BBOB-2023 paper
data_f17/bbobexp_f17_DIM5_i1.dat, 1:5907|4.6e-09, 3:1954|6.4e-09, 5:5339|4.3e-09
suite = 'bbob', funcId = 17, DIM = 10, Precision = 1.000e-08, algId = 's-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% s-CMA-ES: CMA-ES without cumulation for the step size as benchmarked by A. Gissler in his BBOB-2023 paper
data_f17/bbobexp_f17_DIM10_i1.dat, 1:40705|3.9e-09, 3:24484|5.6e-09, 5:23044|5.3e-09
suite = 'bbob', funcId = 17, DIM = 20, Precision = 1.000e-08, algId = 's-CMA-ES', coco_version = '', logger = 'bbob', data_format = 'bbob-new2'
% s-CMA-ES: CMA-ES without cumulation for the step size as benchmarked by A. Gissler in his BBOB-2023 paper
data_f17/bbobexp_f17_DIM20_i1.dat, 1:81437|3.2e-09, 3:86825|3.2e-09, 5:85157|2.4e-09