2013AJ....146...84W


Query : 2013AJ....146...84W

2013AJ....146...84W - Astron. J., 146, 84 (2013/October-0)

The evolution of dusty star formation in galaxy clusters to z = 1: Spitzer infrared observations of the first Red-Sequence Cluster Survey.

WEBB T.M.A., O'DONNELL D., YEE H.K.C., GILBANK D., COPPIN K., ELLINGSON E., FALOON A., GEACH J.E., GLADDERS M., NOBLE A., MUZZIN A., WILSON G. and YAN R.

Abstract (from CDS):

We present the results of an infrared (IR) study of high-redshift galaxy clusters with the MIPS camera on board the Spitzer Space Telescope. We have assembled a sample of 42 clusters from the Red-Sequence Cluster Survey-1 over the redshift range 0.3 < z < 1.0 and spanning an approximate range in mass of 1014–15 M☉. We statistically measure the number of IR-luminous galaxies in clusters above a fixed inferred IR luminosity of 2x1011 M ☉, assuming a star forming galaxy template, per unit cluster mass and find it increases to higher redshift. Fitting a simple power-law we measure evolution of (1 + z)5.1±1.9 over the range 0.3 < z < 1.0. These results are tied to the adoption of a single star forming galaxy template; the presence of active galactic nuclei, and an evolution in their relative contribution to the mid-IR galaxy emission, will alter the overall number counts per cluster and their rate of evolution. Under the star formation assumption we infer the approximate total star formation rate per unit cluster mass (ΣSFR/M cluster). The evolution is similar, with ΣSFR/Mcluster∼ (1 + z)5.4±1.9. We show that this can be accounted for by the evolution of the IR-bright field population over the same redshift range; that is, the evolution can be attributed entirely to the change in the in-falling field galaxy population. We show that the ΣSFR/Mcluster(binned over all redshift) decreases with increasing cluster mass with a slope (ΣSFR/ Mcluster ∼ M–1.5±0.4cluster) consistent with the dependence of the stellar-to-total mass per unit cluster mass seen locally. The inferred star formation seen here could produce ∼5%-10% of the total stellar mass in massive clusters at z = 0, but we cannot constrain the descendant population, nor how rapidly the star-formation must shut-down once the galaxies have entered the cluster environment. Finally, we show a clear decrease in the number of IR-bright galaxies per unit optical galaxy in the cluster cores, confirming star formation continues to avoid the highest density regions of the universe at z ∼ 0.75 (the average redshift of the high-redshift clusters). While several previous studies appear to show enhanced star formation in high-redshift clusters relative to the field we note that these papers have not accounted for the overall increase in galaxy or dark matter density at the location of clusters. Once this is done, clusters at z ∼ 0.75 have the same or less star formation per unit mass or galaxy as the field.

Abstract Copyright: ∼

Journal keyword(s): galaxies: clusters: general - galaxies: evolution - galaxies: starburst - infrared: galaxies

Simbad objects: 43

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Number of rows : 43
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 RCS J022056-0333.3 ClG 02 20 55 -03 33.5           ~ 20 0
2 ACT-CL J0221.9-0340 ClG 02 21 55.5396 -03 40 10.388           ~ 7 0
3 RCS J022359+0126.1 ClG 02 24 00.8 +01 25 55           ~ 4 0
4 RCS J022403-0227.7 ClG 02 24 03.4 -02 27 52           ~ 7 0
5 RCS J022433-0002.3 ClG 02 24 33 -00 02.3           ~ 1 0
6 RCS J022516+0011.5 ClG 02 25 16 +00 11.5           ~ 2 0
7 RCS J035139-0956.4 ClG 03 51 39.5 -09 56 33           ~ 4 0
8 RCS J043938-2904.8 ClG 04 39 38 -29 04.8           ~ 1 0
9 RCS J044126-2813.2 ClG 04 41 26 -28 13.2           ~ 1 0
10 RCS J044207-2815.0 ClG 04 42 08.1 -28 15 11           ~ 1 0
11 RCS J051834-4325.1 ClG 05 18 35.2 -43 25 15           ~ 4 0
12 RCS J051855-4315.0 ClG 05 18 55.0 -43 15 01           ~ 4 0
13 RCS J051908-4323.3 ClG 05 19 08 -43 23.3           ~ 1 0
14 RCS J051940-4402.1 ClG 05 19 40.3 -44 02 14           ~ 4 0
15 RCS J092821+3646.5 ClG 09 28 21.80 +36 46 31.8           ~ 10 0
16 NAME COSMOS Field reg 10 00 28.60 +02 12 21.0           ~ 3639 0
17 RCS J110104-0351.3 ClG 11 01 04.7 -03 51 21           ~ 2 0
18 RCS J110118-0328.6 ClG 11 01 18 -03 28.6           ~ 1 0
19 RCS J110206-0414.5 ClG 11 02 06 -04 14.5           ~ 1 0
20 RCS J110246-0426.9 ClG 11 02 45.9 -04 26 53           ~ 2 0
21 RCS J110411-0337.5 ClG 11 04 11 -03 37.5           ~ 1 0
22 RCS J110439-0445.0 ClG 11 04 40.3 -04 45 03           ~ 4 0
23 RCS J110615-0330.8 ClG 11 06 15 -03 30.8           ~ 1 0
24 RCS J110733-0520.6 ClG 11 07 33.5 -05 20 39           ~ 2 0
25 RCS J112225+2422.9 ClG 11 22 25.5 +24 22 51           ~ 5 0
26 RCS J132631+2903.3 ClG 13 26 31 +29 03.3           ~ 1 0
27 RCS J132655+3021.1 ClG 13 26 55.50 +30 21 11.6           ~ 6 0
28 RCS J132939+2853.3 ClG 13 29 39.40 +28 53 18.2           ~ 3 0
29 ClG J1419+5326 ClG 14 19 10.3 +53 26 08           ~ 24 0
30 RCS J144557+0840.3 ClG 14 45 57 +08 40.3           ~ 1 0
31 RCS J144654+0827.0 ClG 14 46 54 +08 27.0           ~ 3 0
32 ACT-CL J1447.4+0828 ClG 14 47 25.0 +08 27 32           ~ 43 0
33 RCS J145226+0834.6 ClG 14 52 27.3 +08 34 37           ~ 6 0
34 ClG J1620+2929 ClG 16 20 09.4 +29 29 26           ~ 21 0
35 RCS J211852-6334.6 ClG 21 18 52.6 -63 34 43           ~ 2 0
36 RCS J212134-6335.8 ClG 21 21 35.0 -63 35 51           ~ 3 0
37 RCS J212238-6146.1 ClG 21 22 38.3 -61 46 17           ~ 2 0
38 RCS J215223-0503.8 ClG 21 52 23.2 -05 03 44           ~ 4 0
39 RCS J215248-0609.4 ClG 21 52 49.2 -06 09 24           ~ 5 0
40 RCS J231526-0046.7 ClG 23 15 26.7 -00 46 57           ~ 4 0
41 ClG J2319+0038 ClG 23 19 53 +00 38.0           ~ 41 1
42 ACT-CL J2342.3-3534 ClG 23 42 20.4 -35 34 16           ~ 5 0
43 RCS J234717-3634.4 ClG 23 47 17.4 -36 34 33           ~ 3 0

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