suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM2_i1.dat, 1:482|3.6e-09, 3:536|4.9e-10, 5:476|1.6e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM3_i1.dat, 1:919|6.5e-09, 3:1199|1.0e-08, 5:926|7.6e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM5_i1.dat, 1:2442|8.5e-09, 3:2762|9.1e-09, 5:2210|7.7e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM10_i1.dat, 1:8082|9.3e-09, 3:10172|8.4e-09, 5:7722|1.0e-08
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM20_i1.dat, 1:75940|5.3e-09, 3:46408|5.3e-09, 5:33423|5.0e-09