suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM2_i2.dat, 2:14787|1.2e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM3_i2.dat, 2:15501|4.2e-10
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM5_i2.dat, 2:170768|1.8e-09
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM10_i2.dat, 2:422792|9.3e-11
suite = 'bbob', funcId = 19, 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_f19/bbobexp_f19_DIM20_i2.dat, 2:4363611|3.0e-11