suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM2_i4.dat, 4:17|2.3e-13
suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM3_i4.dat, 4:20|2.6e-13
suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM5_i4.dat, 4:25|8.5e-14
suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM10_i4.dat, 4:40|8.5e-14
suite = 'bbob', funcId = 1, 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_f1/bbobexp_f1_DIM20_i4.dat, 4:62|6.5e-13