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 | |||||||
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Centered-halo | 1D | 2D | 2D+vR | 1D | 2D | 2D+vR | 1D | 2D | 2D+vR |
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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 |
|
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Shifted-halo | – | 2D | 2D+vR | – | 2D | 2D+vR | – | 2D | 2D+vR |
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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 | |||||
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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 |
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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 |
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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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