suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM2_i1.dat, 2:3526|1.8e-09, 4:1611|2.7e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM3_i1.dat, 2:6493|5.5e-09, 4:3426|3.3e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM5_i1.dat, 2:10580|4.4e-09, 4:11028|1.5e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM10_i1.dat, 2:24744|4.8e-09, 4:25104|3.2e-09
suite = 'bbob', funcId = 18, 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_f18/bbobexp_f18_DIM20_i1.dat, 2:204030|2.0e-09, 4:185226|2.4e-09