suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM2_i1.dat, 2:476|7.2e-09, 4:422|1.0e-10
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM3_i1.dat, 2:667|4.2e-09, 4:674|1.9e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM5_i1.dat, 2:1402|3.7e-09, 4:1546|9.5e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM10_i1.dat, 2:4872|4.2e-09, 4:4302|7.6e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM20_i1.dat, 2:16562|8.2e-09, 4:15626|5.6e-09