![]() |
![]() |
![]() |
|
c+f | 0.5 (Fig. A.1a) | 0.0 | 0.0 |
![]() |
![]() |
![]() |
|
c | 0.1 | 0.2 | 0.4 |
![]() |
![]() |
![]() |
|
c+f | 0.2 | 0.3 | -0.4 |
c | 0.1 | 0.5 (Fig. 11b) | -0.1 |
MB-k3,5/k1 |
![]() |
![]() |
|
c+f | 0.0 | -0.1 | 0.4 |
c | -0.3 | -0.5 (Fig. 11c) | 0.1 |
A-k3,5/k1 |
![]() |
![]() |
|
c+f | -0.2 | 0.1 | -0.1 |
c | -0.1 | 0.2 | 0.0 |
C-k3,5/k1 |
![]() |
![]() |
|
c+f | 0.0 | -0.1 | 0.2 |
c | 0.1 | 0.0 | -0.2 |
![]() |
![]() |
![]() |
|
c+f | 0.1 | 0.1 | -0.1 |
c | 0.8 (Fig. 10b) | 0.8 (Fig. 10a) | 0.0 |
z-k3,5/k1 |
![]() |
![]() |
|
f | 0.1 | 0.0 | 0.1 |
(B-V)-k3,5/k1 |
![]() |
![]() |
|
c+f | -0.1 | -0.2 | -0.2 |
c | -0.2 | -0.1 | -0.2 |
(V-I)-k3,5/k1 |
![]() |
![]() |
|
c+f | 0.0 | 0.2 | 0.0 |
c | 0.4 | 0.2 | 0.1 |
(R-I)-k3,5/k1 |
![]() |
![]() |
|
c+f | -0.1 | -0.2 | 0.0 |
c | -0.3 | -0.3 | -0.2 |
![]() |
![]() |
![]() |
|
c+f | -0.1 | 0.0 | 0.3 |
c | 0.2 | 0.1 | 0.1 |
M20-k3,5/k1 |
![]() |
![]() |
|
c+f | 0.1 | 0.2 | 0.0 |
c | 0.1 | 0.3 | 0.5 (Fig. 11a) |
![]() |
![]() |
![]() |
|
c+f | -0.3 | -0.2 | -0.4 |
c | -0.2 | 0.0 | -0.3 |
Notes. The
figures where
of the galaxies that have
(galaxies 1F2, 2F4, 2F12 and 4C3
in
``this sample'', NGC 628, NGC 3184, NGC 3938
and NGC 5713 in the local sample),
k3,5/k1
of galaxy 1F5 (this sample) and all parameters for
galaxies 1F10, 2F5, 2F11 and 2F15&16
(this sample) are doubtful as explained in Paper III for the
MS 0451 sample and here, in Sect. 3.8 for the rest.
Therefore, they are
excluded while calculating the correlation coefficients. For the
calculation
of the correlations with the redshift, only field galaxies were used,
so the
results do not have the bias of the environment.
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