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_i2.dat, 2:326|8.9e-11, 4:1683|3.8e-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_i2.dat, 2:42693|1.2e-09, 4:23539|4.7e-10
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_i2.dat, 2:222760|1.8e-10, 4:160984|1.6e-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_i2.dat, 2:1228920|1.0e-10, 4:736039|9.1e-11
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_i2.dat, 2:4001339|2.6e-03, 4:4004243|8.1e-08