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Table 6.

Fitting results of the luminosity functions of M 31 disc and halo GC systems.

GC Double Gaussian Single Gaussian Pa


μ1 σ1 μ2 σ2 μ σ
(1) (2) (3) (4) (5) (6) (7) (8)
BATC g

Disc −8.41 ± 0.05 0.96 ± 0.04 −8.91 ± 0.04 −0.26 ± 0.05 −8.23 ± 0.07 0.99 ± 0.07 0.01%
Halo −7.57 ± 0.11 0.94 ± 0.12 −5.17 ± 0.16 0.45 ± 0.16 −7.34 ± 0.16 1.3 ± 0.16 1.72%

2MASS J
Disc −9.9 ± 0.06 1.1 ± 0.05 −10.46 ± 0.06 0.27 ± 0.06 −9.77 ± 0.07 1.12 ± 0.07 0.17%
Halo −8.09 ± 0.16 0.97 ± 0.09 −7.4 ± 0.11 0.35 ± 0.15 −8.36 ± 0.09 0.88 ± 0.09 9.24%

Notes.

(a)

P is the probability from the F-test. If the P value is low (e.g. 5%), we can conclude that the double-Gaussian model is statistically significantly better than the single-Gaussian model.

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