suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM2_i2.dat, 2:476|5.3e-10, 4:476|5.5e-09
suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM3_i2.dat, 2:905|4.7e-09, 4:961|1.9e-09
suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM5_i2.dat, 2:4403|4.2e-09, 4:2354|1.7e-09
suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM10_i2.dat, 2:6462|6.9e-09, 4:5702|4.5e-09
suite = 'bbob', funcId = 9, 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_f9/bbobexp_f9_DIM20_i2.dat, 2:17486|6.5e-09, 4:44151|7.0e-09