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. Author manuscript; available in PMC: 2017 Mar 15.
Published in final edited form as: Stat Sin. 2016 Apr;26(2):445–464. doi: 10.5705/ss.2014.256

Table 2.

Simulation results for data generated based on the Watt-Strogatz graph with different ratios of the number of individual-specific edges to the number of shared edges. Results are based on 100 replications. The numbers in the brackets are standard errors. CLIME: method of Cai, Liu and Luo (2011); GLASSO: graphical Lasso; JEMGM: method of Guo, Levina, Michailidis et al. (2011); fgland GGL: methods of Danaher, Wang and Witten (2014); MPE: proposed method.

Model(ρ) Method Performance
L1 L2 LF SEN SPE MCC
WS(0) CLIME 29.80(0.23) 13.05(0.19) 87.71(1.96) 0.11(0.03) 0.99(0.00) 0.25(0.02)
GLASSO 29.55(0.25) 12.35(0.08) 79.20(0.47) 0.08(0.01) 0.99(0.00) 0.20(0.01)
JEMGM 29.59(0.46) 11.89(0.27) 74.32(2.50) 0.11(0.04) 1.00(0.00) 0.27(0.03)
FGL 29.45(0.33) 12.43(0.13) 80.10(1.22) 0.10(0.02) 0.99(0.00) 0.23(0.03)
GGL 29.65(0.23) 12.65(0.11) 80.53(0.67) 0.08(0.02) 1.00(0.00) 0.22(0.02)
MPE 28.99(0.22) 12.72(0.12) 84.35(1.11) 0.16(0.01) 1.00(0.00) 0.34(0.01)
WS(1/4) CLIME 42.70(0.35) 14.80(0.19) 102.03(2.08) 0.08(0.02) 0.98(0.01) 0.15(0.01)
GLASSO 42.79(0.58) 14.25(0.07) 95.38(0.49) 0.04(0.00) 0.99(0.00) 0.09(0.00)
JEMGM 43.06(0.60) 13.44(0.17) 84.35(1.75) 0.12(0.02) 0.98(0.00) 0.21(0.01)
FGL 43.33(0.59) 14.31(0.06) 96.24(0.49) 0.06(0.01) 0.98(0.00) 0.11(0.01)
GGL 42.84(0.54) 14.30(0.11) 95.95(0.95) 0.05(0.01) 0.99(0.00) 0.11(0.01)
MPE 42.15(0.39) 14.60(0.11) 100.13(1.16) 0.10(0.00) 0.99(0.00) 0.23(0.01)
WS(1) CLIME 63.27(0.35) 18.64(0.19) 128.83(1.94) 0.04(0.01) 0.99(0.00) 0.08(0.01)
GLASSO 62.94(0.31) 17.85(0.11) 120.11(1.01) 0.02(0.01) 0.99(0.00) 0.04(0.01)
JEMGM 63.67(0.85) 16.82(0.23) 107.53(2.20) 0.07(0.01) 0.98(0.00) 0.12(0.01)
FGL 63.11(0.28) 17.86(0.07) 120.82(0.66) 0.02(0.00) 0.99(0.00) 0.04(0.00)
GGL 63.13(0.35) 17.87(0.12) 120.31(1.05) 0.03(0.01) 0.99(0.01) 0.04(0.01)
MPE 62.89(2.57) 18.18(0.47) 123.98(2.71) 0.08(0.09) 0.98(0.09) 0.15(0.01)