suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM2_i92.dat, 92:11922|1.1e-09
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM3_i92.dat, 92:43875|2.6e-09
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM5_i92.dat, 92:48070|3.3e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM10_i92.dat, 92:413358|1.6e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM20_i92.dat, 92:4005539|2.6e-03
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM40_i92.dat, 92:7791431|3.2e-11