suite = 'bbob', funcId = 24, 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_f24/bbobexp_f24_DIM2_i1.dat, 2:400360|1.0e+00, 4:7241|6.5e-09
suite = 'bbob', funcId = 24, 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_f24/bbobexp_f24_DIM3_i1.dat, 2:600743|2.6e+00, 4:600323|3.0e+00
suite = 'bbob', funcId = 24, 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_f24/bbobexp_f24_DIM5_i1.dat, 2:1000234|3.8e-01, 4:1001290|5.1e+00
suite = 'bbob', funcId = 24, 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_f24/bbobexp_f24_DIM10_i1.dat, 2:2003881|1.1e+00, 4:2004241|5.0e+00
suite = 'bbob', funcId = 24, 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_f24/bbobexp_f24_DIM20_i1.dat, 2:4003487|9.2e+00, 4:4004339|2.0e+01