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_i5.dat, 5:609|5.1e-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_i5.dat, 5:757|6.0e-10
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_i5.dat, 5:1789|2.3e-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_i5.dat, 5:5788|5.4e-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_i5.dat, 5:15581|6.9e-09