suite = 'bbob', funcId = 7, 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_f7/bbobexp_f7_DIM2_i2.dat, 2:242|5.7e-09, 4:531|2.4e-09
suite = 'bbob', funcId = 7, 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_f7/bbobexp_f7_DIM3_i2.dat, 2:366|2.9e-09, 4:759|4.0e-09
suite = 'bbob', funcId = 7, 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_f7/bbobexp_f7_DIM5_i2.dat, 2:1451|3.0e-09, 4:1788|4.5e-09
suite = 'bbob', funcId = 7, 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_f7/bbobexp_f7_DIM10_i2.dat, 2:5144|3.9e-09, 4:2873|9.4e-09
suite = 'bbob', funcId = 7, 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_f7/bbobexp_f7_DIM20_i2.dat, 2:14236|7.9e-09, 4:25301|7.0e-09