suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM2_i92.dat, 92:5412|3.0e-09
suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM3_i92.dat, 92:1207|7.6e-10
suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM5_i92.dat, 92:23855|3.1e-11
suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM10_i92.dat, 92:578531|6.9e-01
suite = 'bbob', funcId = 22, 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_f22/bbobexp_f22_DIM20_i92.dat, 92:1064867|6.9e-01
suite = 'bbob', funcId = 22, DIM = 40, 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_f22/bbobexp_f22_DIM40_i92.dat, 92:2452436|8.7e+00