suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM2_i1.dat, 1:930|9.4e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM3_i1.dat, 1:5239|9.4e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM5_i1.dat, 1:7628|3.6e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM10_i1.dat, 1:14607|6.4e-09
suite = 'bbob', funcId = 13, 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_f13/bbobexp_f13_DIM20_i1.dat, 1:61148|7.0e-09