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_i2.dat, 1:824|3.5e-09, 3:1791|1.3e-09, 5:1875|6.5e-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_i2.dat, 1:4911|2.0e-09, 3:5492|6.3e-09, 5:5380|2.6e-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_i2.dat, 1:44237|3.0e-09, 3:5019|3.8e-09, 5:10244|1.3e-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_i2.dat, 1:43915|5.6e-09, 3:22874|3.2e-09, 5:23384|2.4e-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_i2.dat, 1:198150|3.2e-09, 3:166206|1.9e-09, 5:88025|2.5e-09