suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM2_i2.dat, 2:1852|4.8e-10, 4:3329|2.0e-11
suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM3_i2.dat, 2:4597|1.7e-09, 4:1263|7.4e-10
suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM5_i2.dat, 2:1859|3.4e-10, 4:498|4.3e-09
suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM10_i2.dat, 2:15875|6.6e-11, 4:562061|5.9e-01
suite = 'bbob', funcId = 21, 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_f21/bbobexp_f21_DIM20_i2.dat, 2:1129355|1.9e+00, 4:7383|2.5e-09