Research Article

Enhanced Differential Evolution Algorithm with Local Search Based on Hadamard Matrix

Table 2

Experimental results of four classical operators of DE with HLS for all test functions and comparison without HLS.

FunDE/rand/1/binDE/rand/1/bin + HLSDE/best/1/binDE/best/1/bin + HLSDE/rand-to-best/1/binDE/rand-to-best/1/bin + HLSDE/current-to-best/1/binDE/current-to-best/1/bin + HLS
Mean error ± Std errorMean error ± Std errorMean error ± Std errorMean error ± Std errorMean error ± Std errorMean err ± Std errMean err ± Std errMean err ± Std err

f13.47e − 18 ± 7.66e − 18−1.12E − 112 ± 6.03E − 1121.94e − 12 ± 1.06e − 11-2.94E − 20 ± 1.61E − 193.41e − 106 ± 1.85e − 105+1.70E − 49 ± 9.31E − 494.90e − 108 ± 1.89e − 107+2.90E − 17 ± 1.59E − 16
f26.46e − 11 ± 9.73e − 11−2.30E − 58 ± 1.22E − 571.90e − 04 ± 1.04e − 03≈7.53E − 04 ± 4.09E − 031.83e − 59 ± 7.68e − 59+1.36E − 06 ± 7.47E − 063.55e − 61 ± 1.27e − 60+3.96E − 12 ± 2.17E − 11
f33.46e − 02 ± 3.26e − 02+1.65E + 00 ± 2.73E + 001.55e − 21 ± 4.76e − 21+2.10E − 15 ± 7.15E − 152.86e − 24 ± 7.23e − 24+3.93E − 17 ± 6.83E − 176.53e − 25 ± 1.50e − 24+2.39E + 00 ± 1.31E + 01
f41.53e + 01 ± 7.28e + 00−1.73E − 165 ± 0.00E + 003.60e + 01 ± 7.31e + 00−2.70E − 03 ± 1.45E − 022.23e + 01 ± 5.68e + 00−3.72E − 175 ± 0.00E + 002.63e + 01 ± 7.30e + 00−5.02E − 05 ± 2.12E − 04
f58.83e + 00 ± 3.21e + 00≈1.19E + 01 ± 1.38E + 019.30e − 01 ± 1.71e + 00+2.27E + 01 ± 1.16E + 011.20e + 00 ± 1.86e + 00+2.55E + 01 ± 8.66E + 001.46e + 00 ± 1.95e + 00+2.27E + 01 ± 1.16E + 01
f62.67e − 01 ± 7.85e − 01−0.00E + 00 ± 0.00E + 002.27e + 02 ± 5.80e + 02−0.00E + 00 ± 0.00E + 003.03e + 01 ± 7.46e + 01−0.00E + 00 ± 0.00E + 001.85e + 01 ± 2.45e + 01−0.00E + 00 ± 0.00E + 00
f71.63e − 02 ± 5.98e − 03−3.54E − 03 ± 4.00E − 031.11e − 02 ± 7.48e − 03-2.30E − 03 ± 4.55E − 038.50e − 03 ± 4.20e − 03−1.70E − 03 ± 3.10E − 038.40e − 03 ± 4.20e − 03−1.30E − 03 ± 1.36E − 03
f81.32e + 04 ± 2.47e + 02−1.26E + 04 ± 0.00E + 001.55e + 04 ± 6.80e + 02−1.38E + 04 ± 1.77E + 031.49e + 04 ± 5.66e + 02−1.32E + 04 ± 1.29E + 031.54e + 04 ± 6.62e + 02−1.30E + 04 ± 1.13E + 03
f92.41e + 01 ± 7.72e + 00−0.00E + 00 ± 0.00E + 006.60e + 01 ± 2.03e + 01−1.49E + 01 ± 2.40E + 013.66e + 01 ± 8.98e + 00−2.78E + 00 ± 8.54E + 004.09e + 01 ± 1.12e + 01−6.41E + 00 ± 1.29E + 01
f103.68e − 10 ± 3.02e − 10−4.74E − 16 ± 1.23E − 154.78e + 00 ± 2.44e + 00−3.46E − 01 ± 1.51E + 002.34e + 00 ± 1.35e + 00−3.04E − 14 ± 1.59E − 132.78e + 00 ± 2.04e + 00−2.01E − 15 ± 2.02E − 15
f113.37e − 03 ± 8.55e − 03−0.00E + 00 ± 0.00E + 005.09e − 02 ± 7.59e − 02−1.58E − 02 ± 6.72E − 022.55e − 02 ± 3.08e − 02−3.11E − 03 ± 1.08E − 021.55e − 02 ± 1.95e − 02-5.75E − 04 ± 2.21E − 03
f124.53e − 02 ± 2.29e − 01−1.57E − 32 ± 1.91E − 341.01e + 00 ± 2.15e + 00−3.46E − 03 ± 1.89E − 025.00e − 01 ± 8.89e − 01−1.73E − 02 ± 7.74E − 027.25e − 01 ± 1.00e + 00−1.68E − 32 ± 2.47E − 33
f137.32e − 04 ± 2.79e − 03−1.35E − 32 ± 5.57E − 487.44e − 01 ± 1.70e + 00−3.66E − 04 ± 2.01E − 035.65e − 01 ± 1.49e + 00−4.01E − 32 ± 8.12E − 323.61e − 01 ± 9.67e − 01−3.66E − 04 ± 2.01E − 03
f141.65e − 18 ± 4.20e − 18−0.00E + 00 ± 0.00E + 008.77e − 22 ± 4.80e − 21+1.62E + 01 ± 8.89E + 015.07e − 30 ± 9.73e − 30+4.80E − 05 ± 2.63E − 043.57e − 30 ± 2.69e − 30+4.16E − 17 ± 2.27E − 16
f153.73e − 02 ± 3.54e − 02+1.16E + 00 ± 1.75E + 005.48e − 22 ± 1.45e − 21+1.05E − 15 ± 1.88E − 155.30e − 24 ± 2.06e − 23+1.12E − 06 ± 6.14E − 068.67e − 25 ± 2.10e − 24+7.27E − 17 ± 1.80E − 16
f163.73e − 02 ± 4.47e − 02+2.76E − 01 ± 5.10E − 019.76e − 03 ± 4.36e − 02−1.42E − 05 ± 4.99E − 053.02e − 07 ± 1.17e − 06+3.75E + 00 ± 2.05E + 012.75e − 10 ± 1.34e − 09+8.68E − 07 ± 4.75E − 06
f171.81e − 03 ± 4.92e − 03−0.00E + 00 ± 0.00E + 004.13e − 02 ± 4.73e − 02−7.75E − 03 ± 4.24E − 021.65e − 02 ± 1.65e − 02−2.47E − 04 ± 1.35E − 033.13e − 02 ± 3.18e − 02−0.00E + 00 ± 0.00E + 00
f183.13e − 10 ± 2.45e − 10−3.55E − 16 ± 1.08E − 153.25e + 00 ± 1.95e + 00−1.78E − 03 ± 9.72E − 032.31e + 00 ± 1.19e + 00−1.18E − 15 ± 1.94E − 152.62e + 00 ± 9.67e − 01−1.66E − 15 ± 1.80E − 15
f196.91e − 03 ± 3.79e − 02−1.57E − 32 ± 1.77E − 349.70e − 01 ± 1.87e + 00−1.71E − 32 ± 3.20E − 334.53e − 01 ± 6.95e − 01−1.66E − 32 ± 1.91E − 336.54e − 01 ± 9.23e − 01−3.46E − 03 ± 1.89E − 02
f201.19e − 17 ± 4.41e − 17−1.35E − 32 ± 5.57E − 481.73e + 04 ± 9.47e + 04−1.96E − 31 ± 4.78E − 312.38e − 01 ± 5.94e − 01−6.13E − 32 ± 2.62E − 314.67e − 01 ± 1.63e + 00−6.79E − 32 ± 2.55E − 31

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