suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM2_i2.dat, 2:6328|4.0e-09, 4:3633|2.3e-09
suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM3_i2.dat, 2:27046|3.4e-09, 4:14263|9.3e-09
suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM5_i2.dat, 2:143359|6.8e-09, 4:72678|1.7e-09
suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM10_i2.dat, 2:186366|4.5e-09, 4:2001970|1.9e-02
suite = 'bbob', funcId = 23, 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_f23/bbobexp_f23_DIM20_i2.dat, 2:4005071|7.3e-03, 4:4004399|1.2e+00