suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM2_i2.dat, 1:446|9.9e-09, 3:434|8.0e-09, 5:476|2.0e-09
suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM3_i2.dat, 1:639|1.2e-09, 3:695|9.7e-09, 5:618|8.7e-09
suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM5_i2.dat, 1:1490|9.3e-09, 3:1290|5.5e-09, 5:1098|8.6e-09
suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM10_i2.dat, 1:3982|8.7e-09, 3:4052|9.3e-09, 5:4412|9.2e-09
suite = 'bbob', funcId = 14, 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_f14/bbobexp_f14_DIM20_i2.dat, 1:13898|9.9e-09, 3:13334|9.8e-09, 5:16130|9.7e-09