2021A&A...653A.135O


Query : 2021A&A...653A.135O

2021A&A...653A.135O - Astronomy and Astrophysics, volume 653A, 135-135 (2021/9-1)

Atacama Cosmology Telescope measurements of a large sample of candidates from the Massive and Distant Clusters of WISE Survey. Sunyaev-Zeldovich effect confirmation of MaDCoWS candidates using ACT.

ORLOWSKI-SCHERER J., DI MASCOLO L., BHANDARKAR T., MANDUCA A., MROCZKOWSKI T., AMODEO S., BATTAGLIA N., BRODWIN M., CHOI S.K., DEVLIN M., DICKER S., DUNKLEY J., GONZALEZ A.H., HAN D., HILTON M., HUFFENBERGER K., HUGHES J.P., MacINNIS A., KNOWLES K., KOOPMAN B.J., LOWE I., MOODLEY K., NATI F., NIEMACK M.D., PAGE L.A., PARTRIDGE B., ROMERO C., SALATINO M., SCHILLACI A., SEHGAL N., SIFON C., STAGGS S., STANFORD S.A., THORNTON R., VAVAGIAKIS E.M., WOLLACK E.J., XU Z. and ZHU N.

Abstract (from CDS):


Context. Galaxy clusters are an important tool for cosmology, and their detection and characterization are key goals for current and future surveys. Using data from the Wide-field Infrared Survey Explorer (WISE), the Massive and Distant Clusters of WISE Survey (MaDCoWS) located 2839 significant galaxy overdensities at redshifts 0.7≤z≤1.5, which included extensive follow-up imaging from the Spitzer Space Telescope to determine cluster richnesses. Concurrently, the Atacama Cosmology Telescope (ACT) has produced large area millimeter-wave maps in three frequency bands along with a large catalog of Sunyaev-Zeldovich (SZ)-selected clusters as part of its Data Release 5 (DR5).
Aims. We aim to verify and characterize MaDCoWS clusters using measurements of, or limits on, their thermal SZ effect signatures. We also use these detections to establish the scaling relation between SZ mass and the MaDCoWS-defined richness.
Methods. Using the maps and cluster catalog from DR5, we explore the scaling between SZ mass and cluster richness. We do this by comparing cataloged detections and extracting individual and stacked SZ signals from the MaDCoWS cluster locations. We use complementary radio survey data from the Very Large Array, submillimeter data from Herschel, and ACT 224GHz data to assess the impact of contaminating sources on the SZ signals from both ACT and MaDCoWS clusters. We use a hierarchical Bayesian model to fit the mass-richness scaling relation, allowing for clusters to be drawn from two populations: one, a Gaussian centered on the mass-richness relation, and the other, a Gaussian centered on zero SZ signal.
Results. We find that MaDCoWS clusters have submillimeter contamination that is consistent with a gray-body spectrum, while the ACT clusters are consistent with no submillimeter emission on average. Additionally, the intrinsic radio intensities of ACT clusters are lower than those of MaDCoWS clusters, even when the ACT clusters are restricted to the same redshift range as the MaDCoWS clusters. We find the best-fit ACT SZ mass versus MaDCoWS richness scaling relation has a slope of p1=1.84–0.14+0.15, where the slope is defined as Mλ∝λ15p1 and λ15 is the richness. We also find that the ACT SZ signals for a significant fraction (∼57%) of the MaDCoWS sample can statistically be described as being drawn from a noise-like distribution, indicating that the candidates are possibly dominated by low-mass and unvirialized systems that are below the mass limit of the ACT sample. Further, we note that a large portion of the optically confirmed ACT clusters located in the same volume of the sky as MaDCoWS are not selected by MaDCoWS, indicating that the MaDCoWS sample is not complete with respect to SZ selection. Finally, we find that the radio loud fraction of MaDCoWS clusters increases with richness, while we find no evidence that the submillimeter emission of the MaDCoWS clusters evolves with richness.
Conclusions. We conclude that the original MaDCoWS selection function is not well defined and, as such, reiterate the MaDCoWS collaboration's recommendation that the sample is suited for probing cluster and galaxy evolution, but not cosmological analyses. We find a best-fit mass-richness relation slope that agrees with the published MaDCoWS preliminary results. Additionally, we find that while the approximate level of infill of the ACT and MaDCoWS cluster SZ signals (1-2%) is subdominant to other sources of uncertainty for current generation experiments, characterizing and removing this bias will be critical for next-generation experiments hoping to constrain cluster masses at the sub-percent level.

Abstract Copyright: © ESO 2021

Journal keyword(s): large-scale structure of Universe - cosmic background radiation - submillimeter: galaxies - radio continuum: galaxies - galaxies: clusters: general - galaxies: clusters: intracluster medium

VizieR on-line data: <Available at CDS (J/A+A/653/A135): tablec1.dat>

Simbad objects: 94

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Number of rows : 94
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 ACT-CL J0019.0-0000 ClG 00 18 57.6 +00 00 13           ~ 3 0
2 ACT-CL J0019.8+0210 ClG 00 19 49.88 +02 09 50.2           ~ 4 0
3 ACT-CL J0023.9-0945 ClG 00 24 01.2 -09 44 50           ~ 3 0
4 ACT-CL J0028.1-1005 ClG 00 28 08.35 -10 05 45.9           ~ 3 0
5 ACT-CL J0028.9-4449 ClG 00 28 56.1 -44 49 56           ~ 3 0
6 ACT-CL J0048.4+1757 ClG 00 48 35.62 +17 57 10.2           ~ 3 0
7 ACT-CL J0101.7+0030 ClG 01 01 41.54 +00 30 27.1           ~ 3 0
8 ACT-CL J0102.6+0201 ClG 01 02 39.06 +02 01 18.5           ~ 3 0
9 ACT-CL J0103.7+0119 ClG 01 03 45.7 +01 17 21           ~ 2 0
10 ACT-CL J0105.5+1323 ClG 01 05 31.5 +13 23 55           ~ 7 0
11 ACT-CL J0105.8-1839 ClG 01 05 50.54 -18 39 57.0           ~ 3 0
12 ACT-CL J0120.7-0305 ClG 01 20 41.2 -03 04 32           ~ 3 0
13 ACT-CL J0125.3-0802 ClG 01 25 18.13 -08 02 25.5           ~ 4 0
14 ACT-CL J0129.2-1641 ClG 01 29 11.43 -16 41 02.8           ~ 4 0
15 ACT-CL J0131.9+0329 ClG 01 31 58.71 +03 29 02.5           ~ 3 0
16 ACT-CL J0151.3-4300 ClG 01 51 17.4 -43 00 16           ~ 3 0
17 ACT-CL J0151.4-5954 ClG 01 51 25.2 -59 54 34           ~ 3 0
18 ACT-CL J0200.7-3106 ClG 02 00 45.4 -31 06 17           ~ 3 0
19 ACT-CL J0204.3-1918 ClG 02 04 21.2 -19 18 14           ~ 3 0
20 ACT-CL J0208.1-0935 ClG 02 08 09.35 -09 35 48.2           ~ 3 0
21 ACT-CL J0212.2+0746 ClG 02 12 19.3458 +07 46 49.917           ~ 9 0
22 ACT-CL J0221.0+1755 ClG 02 21 02.7 +17 55 53           ~ 3 0
23 ACT-CL J0234.5-0107 ClG 02 34 34.9 -01 08 28           ~ 7 0
24 ACT-CL J0239.6-1036 ClG 02 39 41.43 -10 35 17.4           ~ 3 0
25 ACT-CL J0244.6-3011 ClG 02 44 40.6 -30 11 39           ~ 4 0
26 ACT-CL J0248.3-4931 ClG 02 48 18.8 -49 30 59           ~ 3 0
27 ACT-CL J0248.4-0925 ClG 02 48 26.8 -09 25 55           ~ 3 0
28 ClG J0256+0006 ClG 02 56 32.9 +00 06 12           ~ 36 0
29 ACT-CL J0300.2+0125 ClG 03 00 10.71 +01 24 49.8           ~ 5 0
30 ACT-CL J0303.6+1857 ClG 03 03 39.57 +18 57 43.3           ~ 3 0
31 ACT-CL J0308.1-2915 ClG 03 08 06.12 -29 15 19.7           ~ 4 0
32 ACT-CL J0319.4-0025 ClG 03 19 24.4 -00 25 21           ~ 8 0
33 ACT-CL J0339.1-3952 ClG 03 39 08.7 -39 52 24           ~ 7 0
34 ACT-CL J0353.3+0832 ClG 03 53 19.60 +08 32 17.4           ~ 3 0
35 ACT-CL J0434.6-3723 ClG 04 34 38.3 -37 23 45           ~ 3 0
36 ACT-CL J0448.4-1705 ClG 04 48 37.80 -17 05 37.3           ~ 4 0
37 ACT-CL J0842.3+0033 ClG 08 42 24.523 +00 32 35.62           ~ 4 0
38 ACT-CL J0856.4+1736 ClG 08 56 24.0 +17 36 14           ~ 3 0
39 ACT-CL J0934.4+1751 ClG 09 34 24.85 +17 51 53.8           ~ 3 0
40 ACT-CL J1004.5+1203 ClG 10 04 37.1 +12 03 10           ~ 3 0
41 ZwCl 1006+1201 ClG 10 08 47.1 +11 47 55     18.0     ~ 70 0
42 ACT-CL J1014.1+0038 ClG 10 14 07.49 +00 38 30.2           ~ 19 0
43 ACT-CL J1029.9+0016 ClG 10 29 55.61 +00 17 02.3           ~ 3 0
44 ACT-CL J1048.7+0743 ClG 10 48 42.69 +07 43 45.0           ~ 3 0
45 ACT-CL J1053.2+1052 ClG 10 53 21.36 +10 52 15.0           ~ 4 0
46 ACT-CL J1106.8+0737 ClG 11 06 52.2 +07 37 12           ~ 3 0
47 ACT-CL J1110.2-0030 ClG 11 10 19.0 -00 30 27           ~ 3 0
48 ACT-CL J1139.3+0154 ClG 11 39 19.6 +01 54 06           ~ 3 0
49 ACT-CL J1142.1+1345 ClG 11 42 08.40 +13 46 11.2           ~ 3 0
50 ACT-CL J1142.7+1527 ClG 11 42 43.9 +15 27 07           ~ 19 0
51 ACT-CL J1149.4+0921 ClG 11 49 26.82 +09 21 46.9           ~ 3 0
52 ACT-CL J1152.3+1652 ClG 11 52 24.0 +16 52 52           ~ 3 0
53 ACT-CL J1205.0+1525 ClG 12 04 59.85 +15 25 21.2           ~ 3 0
54 ACT-CL J1205.3-0245 ClG 12 05 23.2 -02 44 58           ~ 3 0
55 ACT-CL J1208.3+0501 ClG 12 08 22.36 +05 01 50.3           ~ 3 0
56 ACT-CL J1221.5+1604 ClG 12 21 35.0 +16 03 18           ~ 3 0
57 ACT-CL J1241.0+0010 ClG 12 41 00.76 +00 11 50.4           ~ 3 0
58 ACT-CL J1254.9+0947 ClG 12 54 59.6 +09 48 31           ~ 3 0
59 ACT-CL J1303.2+1733 ClG 13 03 15.2 +17 33 14           ~ 3 0
60 ACT-CL J1310.6+1707 ClG 13 10 39.08 +17 07 21.1           ~ 3 0
61 ACT-CL J1322.9-0227 ClG 13 22 56.30 -02 28 15.0           ~ 5 0
62 ACT-CL J1346.2-0142 ClG 13 46 13.3 -01 42 50           ~ 3 0
63 ACT-CL J1354.8+1329 ClG 13 54 51.70 +13 29 36.0           ~ 5 0
64 ACT-CL J1355.8+1607 ClG 13 55 52.20 +16 07 29.8           ~ 3 0
65 ACT-CL J1414.5+0227 ClG 14 14 36.64 +02 27 20.0           ~ 4 0
66 ACT-CL J1418.2+0723 ClG 14 18 14.5 +07 23 44           ~ 3 0
67 ACT-CL J1424.9-0141 ClG 14 24 55.93 -01 41 28.9           ~ 3 0
68 ACT-CL J1426.7+1740 ClG 14 26 40.3 +17 41 03           ~ 3 0
69 ACT-CL J1454.6+0628 ClG 14 54 36.02 +06 28 21.7           ~ 3 0
70 ACT-CL J1455.5+0439 ClG 14 55 32.8 +04 39 49           ~ 3 0
71 ACT-CL J1514.7+1346 ClG 15 14 43.28 +13 46 29.4           ~ 8 0
72 ACT-CL J1521.1+0451 ClG 15 21 04.6 +04 52 08           ~ 5 0
73 ACT-CL J1525.8+1540 ClG 15 25 48.13 +15 41 19.1           ~ 3 0
74 ACT-CL J1536.5+0954 ClG 15 36 35.47 +09 53 44.1           ~ 3 0
75 ACT-CL J1620.1+1340 ClG 16 20 10.94 +13 40 16.1           ~ 3 0
76 ACT-CL J2121.8+0040 ClG 21 21 48.35 +00 40 03.6           ~ 4 0
77 ACT-CL J2140.5+0248 ClG 21 40 34.6 +02 48 58           ~ 3 0
78 ACT-CL J2146.6-0321 ClG 21 46 38.77 -03 20 49.4           ~ 5 0
79 ACT-CL J2204.9-2955 ClG 22 05 01.11 -29 55 54.6           ~ 4 0
80 ACT-CL J2206.5+0906 ClG 22 06 28.6 +09 06 32           ~ 5 0
81 ACT-CL J2231.9+1131 ClG 22 31 53.70 +11 30 36.4           ~ 3 0
82 ACT-CL J2235.0+1321 ClG 22 35 02.3 +13 20 57           ~ 3 0
83 ACT-CL J2241.3-5339 ClG 22 41 17.0 -53 38 44           ~ 3 0
84 MOO J2247+0507 ClG 22 47 15.62 +05 07 49.1           ~ 4 0
85 ACT-CL J2312.0-4844 ClG 23 12 02.8 -48 44 50           ~ 3 0
86 ACT-CL J2316.2+0920 ClG 23 16 16.5 +09 20 40           ~ 3 0
87 ACT-CL J2319.8-1856 ClG 23 19 50.12 -18 56 48.4           ~ 3 0
88 ACT-CL J2320.2-0621 ClG 23 20 16.8 -06 20 32           ~ 4 0
89 ACT-CL J2326.2+0030 ClG 23 26 17.0 +00 30 04           ~ 3 0
90 ACT-CL J2332.6-0014 ClG 23 32 41.4 -00 14 45           ~ 3 0
91 ACT-CL J2332.7-3813 ClG 23 32 46.9 -38 13 41           ~ 3 0
92 ACT-CL J2334.2-4324 ClG 23 34 09.8 -43 24 52           ~ 3 0
93 ACT-CL J2335.3-3256 ClG 23 35 16.6 -32 56 50           ~ 3 0
94 ACT-CL J2358.8+1836 ClG 23 58 48.58 +18 36 38.5           ~ 3 0

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