suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM2_i1.dat, 1:404|9.9e-09, 3:494|5.7e-09, 5:440|2.2e-10
suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM3_i1.dat, 1:716|6.0e-10, 3:702|5.5e-09, 5:576|7.5e-09
suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM5_i1.dat, 1:1346|2.7e-09, 3:1394|7.2e-09, 5:1122|3.7e-09
suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM10_i1.dat, 1:2982|2.5e-09, 3:3112|8.3e-09, 5:3442|9.2e-09
suite = 'bbob', funcId = 11, 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_f11/bbobexp_f11_DIM20_i1.dat, 1:7982|5.8e-09, 3:7262|5.7e-09, 5:8858|7.4e-09