suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM2_i2.dat, 2:4463|1.4e-09, 4:1209|6.9e-10
suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM3_i2.dat, 2:12585|1.5e-09, 4:18977|1.3e-09
suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM5_i2.dat, 2:23334|1.8e-09, 4:38143|6.7e-11
suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM10_i2.dat, 2:1399901|9.9e-01, 4:1390891|2.0e+00
suite = 'bbob', funcId = 3, 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_f3/bbobexp_f3_DIM20_i2.dat, 2:2655407|5.0e+00, 4:2572067|6.0e+00