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Table D.2

Comparisons between the various mass models: halo vs. halo, axisymmetric vs. asymmetric cases, with vs. without the vR component, and centered- vs. shifted-halo.

AICNFW−AICEIN AICPIS−AICEIN AICNFW−AICPIS

Centered-halo 1D 2D 2D+vR 1D 2D 2D+vR 1D 2D 2D+vR

Axisymmetric case 0.24 0.13 0.12 1.5 0.54 0.55 –0.81 –0.42 –0.43
Asymmetric case 0.13 0.01 0.33 0.24 -0.21 –0.22

Shifted-halo 2D 2D+vR 2D 2D+vR 2D 2D+vR

Axisymmetric case 1.90 2.46 0.34 0.63 1.56 1.83
Asymmetric case 2.20 2.69 0.42 0.67 1.79 2.02
AICAxi.−AICAsym. AIC2D−AIC2D + vR AICCentered−halo−AICShifted−halo

EIN 2D 2D+vR Axi. Asym. Axi. Asym.
Centered-halo 1.62 0.72 6.19 5.30 2D 5.77 6.11
Shifted-halo 1.96 1.02 7.74 6.79 2D+vR 7.31 7.60

NFW 2D 2D+vR Axi. Asym. Axi. Asym.
Centered-halo 1.62 0.71 6.20 5.30 2D 3.99 4.03
Shifted-halo 1.66 0.78 7.17 6.30 2D+vR 4.96 5.03

PIS 2D 2D+vR Axi. Asym. Axi. Asym.
Centered-halo 1.83 0.92 6.19 5.28 2D 5.97 6.02
Shifted-halo 1.88 0.97 7.45 6.54 2D+vR 7.23 7.28

Notes. The numbers are the differences of the Akaike Information Criterion (AIC) for each configuration of mass model. A positive difference AICModel1−AICModel2 means that Model2 is more likely than Model1. Differences of the AIC have been normalized to 105.

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