2009ApJ...704..126H


Query : 2009ApJ...704..126H

2009ApJ...704..126H - Astrophys. J., 704, 126-136 (2009/October-2)

LOCUSS: the mid-infrared Butcher-Oemler effect.

HAINES C.P., SMITH G.P., EGAMI E., ELLIS R.S., MORAN S.M., SANDERSON A.J.R., MERLUZZI P., BUSARELLO G. and SMITH R.J.

Abstract (from CDS):

We study the mid-infrared (MIR) properties of galaxies in 30 massive galaxy clusters at 0.02 ≤ z ≤ 0.40, using panoramic Spitzer/MIPS 24 µm and near-infrared data, including 27 new observations from the LoCuSS and ACCESS surveys. This is the largest sample of clusters to date with such high-quality and uniform MIR data covering not only the cluster cores, but extending into the infall regions. We use these data to revisit the so-called Butcher-Oemler (BO) effect, measuring the fraction of massive infrared luminous galaxies (K < K {*} + 1.5, LIR> 5x1010 L☉) within r200, finding a steady increase in the fraction with redshift from ∼3% at z = 0.02 to ∼10% by z = 0.30, and an rms cluster-to-cluster scatter about this trend of 0.03. The best-fit redshift evolution model of the form fSF∝ (1 + z)^ n ^ has n = 5.7+2.1–1.8, which is stronger redshift evolution than that of L {*}IR in both clusters and the field. We find that, statistically, this excess is associated with galaxies found at large cluster-centric radii, specifically r500< r < r200, implying that the MIR BO effect can be explained by a combination of both the global decline in star formation in the universe since z ∼ 1 and enhanced star formation in the infall regions of clusters at intermediate redshifts. This picture is supported by a simple infall model based on the Millennium Simulation semianalytic galaxy catalogs, whereby star formation in infalling galaxies is instantaneously quenched upon their first passage through the cluster, in that the observed radial trends of fSF trace those inferred from the simulations. The observed fSFvalues, however, lie systematically above the predictions, suggesting an overall excess of star formation, either due to triggering by environmental processes, or a gradual quenching. We also find that fSF does not depend on simple indicators of the dynamical state of clusters, including the offset between the brightest cluster galaxy and the peak of the X-ray emission. This is consistent with the picture described above in that most new star formation in clusters occurs in the infall regions, and is thus not sensitive to the details of cluster-cluster mergers in the core regions.

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Journal keyword(s): galaxies: active - galaxies: clusters: general - galaxies: evolution - galaxies: stellar content

Simbad objects: 36

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Number of rows : 36
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 ZwCl 0024+1652 ClG 00 26 35.6 +17 09 32     18.35     ~ 648 1
2 ZwCl 0104+0048 ClG 01 06 50.5 +01 04 10           ~ 67 0
3 NAME XMM-LSS Field reg 02 18 00 -07 00.0           ~ 347 0
4 ACO 3358 ClG 05 38 14 -20 37.3           ~ 24 0
5 ACO 586 ClG 07 32 20.3 +31 37 58           ~ 196 0
6 ACO 611 ClG 08 00 58.7 +36 02 49           ~ 275 0
7 ZwCl 0823+0425 ClG 08 25 57.8 +04 14 48           ~ 42 0
8 ACO 665 ClG 08 30 45.2 +65 52 55           ~ 457 0
9 ACO 689 ClG 08 37 29 +14 59.5           ~ 53 0
10 ZwCl 0839+2937 ClG 08 42 55.9 +29 27 26     17.0     ~ 93 0
11 ACO 697 ClG 08 42 57.6 +36 21 45           ~ 277 0
12 ZwCl 0857+2107 ClG 09 00 36.90 +20 53 40.3           ~ 103 0
13 NAME Lockman Hole reg 10 45 00.0 +58 00 00           ~ 910 0
14 ACO 1367 ClG 11 44 44.6 +19 41 59           ~ 1127 1
15 ACO 1656 ClG 12 59 44.40 +27 54 44.9           ~ 5141 2
16 NAME Shapley Supercluster SCG 13 06.0 -33 04           ~ 677 0
17 ACO 1689 ClG 13 11 29.5 -01 20 28           ~ 1178 0
18 ACO 3556 ClG 13 24 06.2 -31 39 38           ~ 159 0
19 ACO 3558 ClG 13 28 03.2 -31 31 35           ~ 476 2
20 BAX 202.4458-31.6081 ClG 13 29 47.0 -31 36 29           ~ 80 1
21 BAX 202.9000-31.8128 ClG 13 31 28.8 -31 49 40           ~ 88 1
22 ACO 1758 ClG 13 32 32.1 +50 30 37           ~ 266 2
23 NAME ACO 1758S GrG 13 32 32.8 +50 24 48           ~ 74 0
24 MCXC J1332.7+5032 ClG 13 32 44.8 +50 32 24           ~ 134 0
25 ACO 3562 ClG 13 33 31.8 -31 40 23           ~ 337 1
26 ACO 1763 ClG 13 35 20.1 +41 00 04           ~ 335 0
27 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 727 1
28 ACO 1914 ClG 14 25 57.4 +37 49 54           ~ 338 0
29 ZwCl 1455+2232 ClG 14 57 15.2 +22 20 30     18.62 20.04   ~ 309 0
30 ACO 2218 ClG 16 35 54.0 +66 13 00           ~ 827 1
31 ACO 2219 ClG 16 40 22.1 +46 42 20           ~ 381 0
32 ClG J1720+2638 ClG 17 20 09.6 +26 37 35           ~ 284 0
33 ACO 2345 ClG 21 27 05.391 -12 09 07.41           ~ 151 0
34 NVSS J212709-120958 Rad 21 27 09.27 -12 10 01.5           ~ 132 1
35 ClG J2129+0005 ClG 21 29 40.5 +00 05 47           ~ 308 0
36 ACO 2390 ClG 21 53 37.4 +17 41 46           ~ 732 2

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