suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM2_i2.dat, 1:374|7.3e-09, 3:410|2.5e-10, 5:470|1.4e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM3_i2.dat, 1:793|8.7e-09, 3:646|6.8e-09, 5:604|8.6e-10
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM5_i2.dat, 1:1506|3.8e-09, 3:1218|3.3e-09, 5:1522|7.0e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM10_i2.dat, 1:4592|9.7e-09, 3:4392|3.8e-09, 5:4422|7.3e-09
suite = 'bbob', funcId = 2, 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_f2/bbobexp_f2_DIM20_i2.dat, 1:17042|8.1e-09, 3:17306|4.6e-09, 5:16322|6.7e-09