suite = 'bbob', funcId = 10, DIM = 2, Precision = 1.000e-08, algId = 'SLSQP+lq-CMA-ES', coco_version = '2.3.6', logger = 'bbob', data_format = 'bbob-new2'
% SLSQP+lq-CMA-ES: one run of SLSQP followed with lq-CMA-ES (IPOP mode) from N. Hansen's GECCO 2019 paper, https://hal.inria.fr/hal-02143961/document (2nd continuous COCO submission)
data_f10/bbobexp_f10_DIM2_i80.dat, 80:564|2.9e-09
suite = 'bbob', funcId = 10, DIM = 3, Precision = 1.000e-08, algId = 'SLSQP+lq-CMA-ES', coco_version = '2.3.6', logger = 'bbob', data_format = 'bbob-new2'
% SLSQP+lq-CMA-ES: one run of SLSQP followed with lq-CMA-ES (IPOP mode) from N. Hansen's GECCO 2019 paper, https://hal.inria.fr/hal-02143961/document (2nd continuous COCO submission)
data_f10/bbobexp_f10_DIM3_i80.dat, 80:5200|4.7e-09
suite = 'bbob', funcId = 10, DIM = 5, Precision = 1.000e-08, algId = 'SLSQP+lq-CMA-ES', coco_version = '2.3.6', logger = 'bbob', data_format = 'bbob-new2'
% SLSQP+lq-CMA-ES: one run of SLSQP followed with lq-CMA-ES (IPOP mode) from N. Hansen's GECCO 2019 paper, https://hal.inria.fr/hal-02143961/document (2nd continuous COCO submission)
data_f10/bbobexp_f10_DIM5_i80.dat, 80:6211|3.7e-09
suite = 'bbob', funcId = 10, DIM = 10, Precision = 1.000e-08, algId = 'SLSQP+lq-CMA-ES', coco_version = '2.3.6', logger = 'bbob', data_format = 'bbob-new2'
% SLSQP+lq-CMA-ES: one run of SLSQP followed with lq-CMA-ES (IPOP mode) from N. Hansen's GECCO 2019 paper, https://hal.inria.fr/hal-02143961/document (2nd continuous COCO submission)
data_f10/bbobexp_f10_DIM10_i80.dat, 80:4589|7.0e-09
suite = 'bbob', funcId = 10, DIM = 20, Precision = 1.000e-08, algId = 'SLSQP+lq-CMA-ES', coco_version = '2.3.6', logger = 'bbob', data_format = 'bbob-new2'
% SLSQP+lq-CMA-ES: one run of SLSQP followed with lq-CMA-ES (IPOP mode) from N. Hansen's GECCO 2019 paper, https://hal.inria.fr/hal-02143961/document (2nd continuous COCO submission)
data_f10/bbobexp_f10_DIM20_i80.dat, 80:16280|5.9e-09