suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM2_i1.dat, 2:548|6.7e-10, 4:1046|9.0e-09
suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM3_i1.dat, 2:2613|8.4e-09, 4:2585|5.2e-09
suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM5_i1.dat, 2:1410|6.7e-09, 4:1642|2.1e-09
suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM10_i1.dat, 2:9192|8.8e-09, 4:8312|8.9e-09
suite = 'bbob', funcId = 12, 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_f12/bbobexp_f12_DIM20_i1.dat, 2:23006|9.4e-09, 4:22466|9.9e-09