2001AJ....122.1084L


Query : 2001AJ....122.1084L

2001AJ....122.1084L - Astron. J., 122, 1084-1103 (2001/September-0)

The Tolman surface brightness test for the reality of the expansion. IV. A measurement of the Tolman signal and the luminosity evolution of early-type galaxies.

LUBIN L.M. and SANDAGE A.

Abstract (from CDS):

We review a sample of the early literature in which the reality of the expansion is discussed. Hubble's reluctance, even as late as 1953, to accept the expansion as real is explained as due to his use of equations for distances and absolute magnitudes of redshifted galaxies that do not conform to the modern Mattig equations of the standard model. The Tolman surface brightness test, once the only known test for the reality of the expansion, is contrasted with three other modern tests. These are (1) the time dilation in Type Ia supernovae light curves, (2) the temperature of the relic radiation as a function of redshift, and (3) the surface brightness normalization of the Planckian shape of the relic radiation. We search for the Tolman surface brightness depression with redshift using the Hubble Space Telescope (HST) data from (ref???)Paper III for 34 early-type galaxies from the three clusters Cl 1324+3011 (z=0.76), Cl 1604+4304 (z=0.90), and Cl 1604+4321 (z=0.92). Depressions of the surface brightness relative to the zero-redshift fiducial lines in the mean surface brightness-logarithm of the linear radius diagrams of (ref???)Paper I are found for all three clusters. Expressed as the exponent, n, in 2.5log(1+z)n mag, the value of n averaged over Petrosian radii of η=1.7 and η=2.0 for all three clusters is n=2.59±0.17 in the R band and 3.37±0.13 in the I band for a q0=1/2 model. The sensitivity of the result to the assumed value of q0 is shown to be less than 23% between q=0 and +1. The conclusion is that the exponent on (1+z) varies from 2.28 to 2.81(±0.17) in the R band and 3.06 to 3.55(±0.13) in the I band, depending on the value of q0. For a true Tolman signal with n=4, the luminosity evolution in the look-back time, expressed as the exponent in 2.5log(1+z)^4-n^ mag, must then be between 1.72 to 1.19(±0.17) in the R band and 0.94 to 0.45(±0.13) in the I band. We show that this is precisely the range expected from the evolutionary models of Bruzual and Charlot and other measurements of the luminosity evolution of early-type galaxies. We conclude that the Tolman surface brightness test is consistent with the reality of the expansion to within the combined errors of the observed <SB> depression and the theoretical correction for luminosity evolution. We have also used the high-redshift HST data to test the ``tired light'' speculation for a nonexpansion model for the redshift. The HST data rule out the tired light model at a significance level of better than 10 σ.

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Journal keyword(s): Cosmology: Observations - Galaxies: Clusters: General

Simbad objects: 41

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Number of rows : 41
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
2 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
3 ClG 1322+3027 ClG 13 24 48.2 +30 11 34           ~ 68 0
4 ClG 1603+4313 ClG 16 04 23.7 +43 04 52           ~ 134 1
5 ClG 1603+4329 SCG 16 04 31.5 +43 21 17           ~ 35 1
6 ClG 1602.9+4329 ClG 16 04 35.3 +43 21 02           ~ 50 1
7 NGC 6822 G 19 44 56.199 -14 47 51.29   18 8.1     ~ 1661 0
8 [LS2001] Cl J1604+4321 49 GiC ~ ~           ~ 2 0
9 [LS2001] Cl J1604+4321 112 GiC ~ ~           ~ 2 0
10 [LS2001] Cl J1604+4321 46 GiC ~ ~           ~ 2 0
11 [LS2001] Cl J1604+4321 57 GiC ~ ~           ~ 2 0
12 [LS2001] Cl J1324+3011 9 GiC ~ ~           ~ 2 0
13 [LS2001] Cl J1604+4304 9 GiC ~ ~           ~ 2 0
14 [LS2001] Cl J1324+3011 29 GiC ~ ~           ~ 2 0
15 [LS2001] Cl J1604+4304 46 GiC ~ ~           ~ 2 0
16 [LS2001] Cl J1604+4321 115 GiC ~ ~           ~ 2 0
17 [LS2001] Cl J1324+3011 69 GiC ~ ~     24.29     ~ 3 0
18 [LS2001] Cl J1604+4304 50 GiC ~ ~           ~ 2 0
19 [LS2001] Cl J1604+4321 23 GiC ~ ~           ~ 2 0
20 [LS2001] Cl J1604+4321 78 GiC ~ ~           ~ 2 0
21 [LS2001] Cl J1324+3011 12 GiC ~ ~           ~ 2 0
22 [LS2001] Cl J1324+3011 55 GiC ~ ~           ~ 2 0
23 [LS2001] Cl J1604+4304 10 GiC ~ ~           ~ 2 0
24 [LS2001] Cl J1604+4321 58 GiC ~ ~           ~ 2 0
25 [LS2001] Cl J1324+3011 40 GiC ~ ~   25.91 23.98     ~ 3 0
26 [LS2001] Cl J1324+3011 11 GiC ~ ~           ~ 2 0
27 [LS2001] Cl J1324+3011 74 GiC ~ ~           ~ 2 0
28 [LS2001] Cl J1604+4321 36 GiC ~ ~           ~ 2 0
29 [LS2001] Cl J1604+4321 65 GiC ~ ~           ~ 2 0
30 [LS2001] Cl J1604+4321 144 GiC ~ ~           ~ 2 0
31 [LS2001] Cl J1604+4304 13 GiC ~ ~           ~ 2 0
32 [LS2001] Cl J1604+4304 58 GiC ~ ~           ~ 2 0
33 [LS2001] Cl J1324+3011 18 GiC ~ ~   25.25 22.14     ~ 3 0
34 [LS2001] Cl J1324+3011 59 GiC ~ ~           ~ 2 0
35 [LS2001] Cl J1324+3011 21 GiC ~ ~           ~ 2 0
36 [LS2001] Cl J1324+3011 30 GiC ~ ~           ~ 2 0
37 [LS2001] Cl J1604+4304 34 GiC ~ ~           ~ 2 0
38 [LS2001] Cl J1604+4321 38 GiC ~ ~           ~ 2 0
39 [LS2001] Cl J1604+4321 29 GiC ~ ~           ~ 2 0
40 [LS2001] Cl J1324+3011 26 GiC ~ ~           ~ 2 0
41 [LS2001] Cl J1604+4321 44 GiC ~ ~           ~ 2 0

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