suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM2_i2.dat, 1:7338|2.6e-09, 3:9564|1.4e-09, 5:1467|1.4e-10
suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM3_i2.dat, 1:24059|4.7e-10, 3:13390|2.3e-09, 5:6830|8.0e-10
suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM5_i2.dat, 1:13637|4.5e-10, 3:43039|2.0e-10, 5:90136|2.0e-10
suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM10_i2.dat, 1:361059|2.3e-10, 3:789150|7.2e-11, 5:347159|1.1e-10
suite = 'bbob', funcId = 20, 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_f20/bbobexp_f20_DIM20_i2.dat, 1:4005695|5.9e-02, 3:4005131|1.2e-01, 5:1756690|7.0e-11