Table 6
Modeled parameters of the three different mass model approaches. Top – model with Faber-Jackson scaling relation, middle – model with fundamental plane scaling relation and bottom – our final model with explicitly included X-rays gas mass plus fundamental plane scaling relations.
System | Δα | Δδ | ϵ | θ a | r core | r cut | σ 0 | |
(′′) | (′′) | (kpc) | (′′) | (km s-1) | ||||
|
||||||||
FJ log(Evidence) = –35.1 | rmsFJ = 0.197 ′′ | |||||||
|
||||||||
DM 1 | 8.3 ± 0.3 | −2.5 ± 0.8 | 0.64 ± 0.05 | 72.0 ± 2.1 | 117.4 ± 5.9 | [1000.0] | 884.2 ± 31.9 | |
DM 2 | 24.2 ± 1.0 | 28.3 ± 1.2 | 0.13 ± 0.11 | 56.6 ± 1.0 | 127.3 ± 17.1 | [1000.0] | 840.2 ± 37.5 | |
DM 3 | 185.9 ± 0.3 | 50.1 ± 0.1 | 0.46 ± 0.05 | 5.2 ± 0.5 | 47.3 ± 0.9 | [1000.0] | 795.7 ± 18.9 | |
BCG 1 | [0.00] | [0.00] | [0.26] | [43.5] | [0.3] | 150.0 ± 2.1 | 255.9 ± 39.3 | |
BCG 2 | [24.05] | [29.13] | [0.20] | [37.4] | [0.2] | 112.2 ± 1.8 | 201.6 ± 2.4 | |
Gal A | [51.94] | [48.93] | [0.13] | [9.9] | [0.1] | 60.0 ± 0.9 | 199.3 ± 3.9 | |
Gal B | [5.23] | [23.01] | [0.10] | [−49.0] | [0.1] | 53.3 ± 1.3 | 105.1 ± 1.6 | |
![]() |
... | ... | ... | ... | [0.1] | 48.6 ± 8.5 | 119.2 ± 5.1 | |
|
||||||||
FP log(Evidence) = –34.0 | rmsFP = 0.160 ′′ | |||||||
|
||||||||
DM 1 | 8.2 ± 0.3 | −2.3 ± 0.7 | 0.56 ± 0.07 | 72.4 ± 2.6 | 125.8 ± 7.0 | [1000.0] | 938.1 ± 39.0 | |
DM 2 | 24.8 ± 0.8 | 27.9 ± 1.0 | 0.23 ± 0.09 | 55.4 ± 1.1 | 133.4 ± 7.6 | [1000.0] | 847.0 ± 42.0 | |
DM 3 | 186.0 ± 0.4 | 50.1 ± 0.1 | 0.44 ± 0.04 | 4.8 ± 0.5 | 50.0 ± 3.0 | [1000.0] | 815.2 ± 16.8 | |
BCG 1 | [0.00] | [0.00] | [0.26] | [43.5] | [0.3] | 50.5 ± 12.3 | 201.8 ± 32.0 | |
BCG 2 | [24.05] | [29.13] | [0.20] | [37.4] | [0.2] | 48.8 ± 5.8 | 212.7 ± 7.2 | |
Gal A | [51.94] | [48.93] | [0.13] | [9.9] | [0.1] | 48.1 ± 10.1 | 230.5 ± 4.9 | |
Gal B | [5.23] | [23.01] | [0.10] | [−49.0] | [0.1] | 48.5 ± 2.2 | 117.2 ± 13.1 | |
S FP | ... | ... | ... | ... | [0.1] | 71.1 ± 5.1 | 1.16 ± 0.14b | |
|
||||||||
FP log(Evidence) = –31.7 | rmsFP + X = 0.147 ′′ | |||||||
|
||||||||
DM 1 | 9.6 ± 0.4 | −1.6 ± 1.6 | 0.41 ± 0.06 | 81.7 ± 3.8 | 131.2 ± 12.3 | [1000.0] | 918.6 ± 49.6 | |
DM 2 | 21.6 ± 1.2 | 25.6 ± 2.1 | 0.43 ± 0.07 | 64.5 ± 1.8 | 108.5 ± 12.5 | [1000.0] | 733.0 ± 54.9 | |
DM 3 | 185.6 ± 0.3 | 50.1 ± 0.1 | 0.30 ± 0.02 | 3.5 ± 0.7 | 58.9 ± 1.2 | [1000.0] | 862.2 ± 7.0 | |
BCG 1 | [0.00] | [0.00] | [0.26] | [43.5] | [0.3] | 49.2 ± 5.8 | 302.3 ± 10.5 | |
BCG 2 | [24.05] | [29.13] | [0.20] | [37.4] | [0.2] | 50.3 ± 7.2 | 215.5 ± 7.6 | |
Gal A | [51.94] | [48.93] | [0.13] | [9.9] | [0.1] | 49.5 ± 6.8 | 224.4 ± 5.8 | |
Gal B | [5.23] | [23.01] | [0.10] | [−49.0] | [0.1] | 51.4 ± 7.0 | 117.5 ± 13.5 | |
SFP | ... | ... | ... | ... | [0.1] | 93.1 ± 59.3 | 1.19 ± 0.76b |
Notes. Values quoted within brackets were kept fixed in the optimization. The error bars correspond to 68% confidence levels. The location and the ellipticity of the matter clumps associated with the cluster galaxies were kept fixed according to the light distribution. The ellipticity ϵ is the one of the mass distribution, expressed as a2−b2/a2 + b2. The center is defined at α = 104.6588589δ = −55.9571863 in J2000 coordinates corresponding to the center of the first BCG.
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