suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM2_i1.dat, 1:4024|1.8e-09, 3:1203|2.9e-09, 5:2554|3.4e-09
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM3_i1.dat, 1:33977|6.1e-10, 3:56917|9.5e-10, 5:59563|8.1e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM5_i1.dat, 1:153744|7.9e-11, 3:209104|3.2e-10, 5:96167|5.4e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM10_i1.dat, 1:395008|2.1e-10, 3:668249|6.8e-11, 5:725509|2.2e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM20_i1.dat, 1:4004795|1.4e-02, 3:2014402|1.0e-10, 5:1854778|1.1e-10