Detailed spectral energy distributions, such as those reported here,
will always be
confined to a small sample of galaxies. The much larger amount of
statistical data
required for a thorough study of distant galaxies and clusters of
galaxies must depend on broad-band photometry. Recently
Whitford (1971) and
Schild and Oke (1971)
have computed K-corrections and B - V and V -
RS colors as a function of the redshift out
to z = 0.28, assuming the observed energy distribution for nearby
giant elliptical
galaxies. Schild and Oke have extended the V - RS
calculation to z = 0.60. The present
results for 3C 295 have been matched to the nearby galaxy data and used
to extend the
energy distribution much farther to the violet. The emission in
3727
is omitted in the
combined energy distribution. This new energy distribution has been used
to compute
K-corrections and B - V and V - RS
colors to large values of z. The results for z
0.20
are given in Table 1; for z < 0.20 the
previous results of Schild and Oke (1971) apply.
It is of note that the value of B - V reaches a maximum value at z = 0.24 and then decreases again. Similarly, a maximum value of V - RS occurs at z = 0.50. Inspection of the normalized (B - V)c and (V - RS)c colors indicates that as long as no evolutionary effects on colors occur - and this appears to be the case out to z = 0.46 - the B - V and V - RS colors can be used to predict z. The most sensitive indicator is B - V for z < 0.16. If z lies between 0.16 and 0.48, V - RS will give the redshift. The technique will be most valuable for clusters of galaxies where colors of several galaxies can be measured.
z | KB | KV | KRS | (B - V)c | (V - RS)c |
0.00 | 0.00 | 0.00 | 0.00 | 0.97 | 0.82 |
0.20 | 0.96 | 0.39 | 0.22 | 1.54 | 0.99 |
0.24 | 1.11 | 0.53 | 0.27 | 1.55 | 1.08 |
0.28 | 1.26 | 0.70 | 0.29 | 1.53 | 1.23 |
0.32 | 1.41 | 0.88 | 0.33 | 1.50 | 1.37 |
0.36 | 1.55 | 1.08 | 0.38 | 1.44 | 1.52 |
0.40 | 1.69 | 1.25 | 0.45 | 1.41 | 1.62 |
0.44 | 1.83 | 1.41 | 0.54 | 1.39 | 1.69 |
0.48 | 1.96 | 1.55 | 0.64 | 1.38 | 1.73 |
0.52 | (2.08) | 1.65 | 0.74 | (1.40) | 1.73 |
0.56 | ... | 1.74 | 0.86 | ... | 1.70 |
0.60 | ... | 1.83 | 1.00 | ... | 1.65 |
0.64 | ... | 1.93 | 1.13 | ... | 1.62 |
0.68 | ... | 2.05 | 1.26 | ... | 1.61 |
0.72 | ... | 2.18 | 1.38 | ... | 1.62 |
* Determined by using NGC 4472, NGC 4486, and 3C 295. |
Part of this work was supported by the National Aeronautics and Space Administration through grant NGL-05-002-134.