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_i2.dat, 2:602|7.4e-09, 4:560|5.7e-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_i2.dat, 2:1339|6.6e-09, 4:1038|8.8e-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_i2.dat, 2:2042|6.9e-09, 4:2474|9.2e-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_i2.dat, 2:16033|7.6e-09, 4:12582|6.9e-09
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_i2.dat, 2:53236|3.9e-09, 4:113861|3.3e-09