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_i1.dat, 2:2362|3.1e-09, 4:981|9.9e-09
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_i1.dat, 2:12473|1.3e-09, 4:6480|1.3e-09
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_i1.dat, 2:13613|3.3e-10, 4:13141|3.1e-09
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_i1.dat, 2:179638|1.9e-10, 4:348099|1.2e-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_i1.dat, 2:1811086|6.0e-11, 4:4004255|3.5e-07