2019MNRAS.486.1332K


Query : 2019MNRAS.486.1332K

2019MNRAS.486.1332K - Mon. Not. R. Astron. Soc., 486, 1332-1349 (2019/June-2)

GMRT 610 MHz observations of galaxy clusters in the ACT equatorial sample.

KNOWLES K., BAKER A.J., BOND J.R., GALLARDO P.A., GUPTA N., HILTON M., HUGHES J.P., INTEMA H., LOPEZ-CARABALLO C.H., MOODLEY K., SCHMITT B.L., SIEVERS J., SIFON C. and WOLLACK E.

Abstract (from CDS):

We present Giant Metrewave Radio Telescope (GMRT) 610 MHz observations of 14 Atacama Cosmology Telescope (ACT) clusters, including new data for nine. The sample includes 73 per cent of ACT equatorial clusters with M500 > 5 x 1014 M☉. We detect diffuse emission in three of these (27+20–14 per cent): we detect a radio minihalo in ACT-CL J0022.2-0036 at z = 0.8, making it the highest redshift minihalo known; we detect potential radio relic emission in ACT-CL J0014.9-0057 (z = 0.533); and we confirm the presence of a radio halo in low-mass cluster ACT-CL J0256.5+0006, with flux density S610 = 6.3 ± 0.4 mJy. We also detect residual diffuse emission in ACT-CL J0045.9-0152 (z = 0.545), which we cannot conclusively classify. For systems lacking diffuse radio emission, we determine radio halo upper limits in two ways and find via survival analysis that these limits do not significantly affect radio power scaling relations. Several clusters with no diffuse emission detection are known or suspected mergers, based on archival X-ray and/or optical measures; given the limited sensitivity of our observations, deeper observations of these disturbed systems are required in order to rule out the presence of diffuse emission consistent with known scaling relations. In parallel with our diffuse emission results, we present catalogues of individual radio sources, including a few interesting extended sources. Our study represents the first step towards probing the occurrence of diffuse emission in high-redshift (z >= 0.5) clusters, and serves as a pilot for statistical studies of larger cluster samples with the new radio telescopes available in the pre-SKA era.

Abstract Copyright: © 2019 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): catalogues - galaxies: clusters: general - galaxies: clusters: intracluster medium - radio continuum: galaxies - radio continuum: general

Nomenclature: Figs 1, 3-11, Tables 3, 5-13: [KBB2019] ACT-CL JHHMM.m+DDMM A N=50, [KBB2019] ACT-CL JHHMM.m+DDMM WW N=3, [KBB2019] ACT-CL J0256.5+0006 RH N=1, [KBB2019] ACT-CL J0014.9-0057 CE N=1.

Simbad objects: 75

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Number of rows : 75
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 [KBB2019] ACT-CL J0014.9-0057 D Rad 00 14 49.275 -00 56 39.87           ~ 1 0
2 [KBB2019] ACT-CL J0014.9-0057 NW Rad 00 14 51.079 -00 56 13.80           ~ 1 0
3 SDSS J001451.57-005744.5 rG 00 14 51.5760 -00 57 44.574           ~ 3 0
4 NVSS J001452-005719 rG 00 14 52.3690 -00 57 20.029           ~ 3 0
5 ACT-CL J0014.9-0057 ClG 00 14 54.105 -00 57 08.24           ~ 18 0
6 SDSS J001454.10-005708.4 rG 00 14 54.107 -00 57 08.48           ~ 5 0
7 [KBB2019] ACT-CL J0014.9-0057 CE Rad 00 14 54.138 -00 57 01.69           ~ 1 0
8 SDSS J001456.63-005635.3 rG 00 14 56.635 -00 56 35.31           ~ 5 0
9 [KBB2019] ACT-CL J0022.2-0036 E Rad 00 22 09.827 -00 36 43.95           ~ 1 0
10 SDSS J002212.75-003612.5 rG 00 22 12.759 -00 36 12.51           ~ 4 0
11 ACT-CL J0022-0036 ClG 00 22 13.00 -00 36 33.8           ~ 16 0
12 NVSS J002213-003632 rG 00 22 13.03414 -00 36 33.9591           ~ 3 0
13 SDSS J002213.29-003604.6 Rad 00 22 13.290 -00 36 04.65           ~ 2 0
14 [KBB2019] ACT-CL J0022.2-0036 A Rad 00 22 17.153 -00 36 31.61           ~ 1 0
15 [KBB2019] ACT-CL J0045.2-0152 C Rad 00 45 10.208 -01 52 12.42           ~ 1 0
16 [KBB2019] ACT-CL J0045.2-0152 NW Rad 00 45 10.916 -01 52 15.18           ~ 1 0
17 SDSS J004511.50-015309.6 rG 00 45 11.508 -01 53 09.64           ~ 4 0
18 SDSS J004512.49-015231.6 rG 00 45 12.500 -01 52 31.66           ~ 5 0
19 ACT-CL J0045.2-0152 ClG 00 45 12.50 -01 52 31.6           ~ 21 0
20 [KBB2019] ACT-CL J0045.2-0152 F Rad 00 45 12.552 -01 52 53.92           ~ 1 0
21 [KBB2019] ACT-CL J0045.2-0152 SE Rad 00 45 14.197 -01 52 59.74           ~ 1 0
22 [KBB2019] ACT-CL J0045.2-0152 D Rad 00 45 15.005 -01 52 58.96           ~ 1 0
23 [KBB2019] ACT-CL J0045.2-0152 A Rad 00 45 15.288 -01 51 58.28           ~ 1 0
24 SDSS J004515.94-015340.0 rG 00 45 15.949 -01 53 40.05           ~ 4 0
25 NGC 245 EmG 00 46 05.395 -01 43 24.21   13.7   13.3 12.9 ~ 97 0
26 ACT-CL J0059.1-0049 ClG 00 59 08.50 -00 50 05.7           ~ 14 0
27 SDSS J005908.50-005005.7 Rad 00 59 08.500 -00 50 05.79           ~ 2 0
28 [KBB2019] ACT-CL J0059.1-0049 A Rad 00 59 08.782 -00 49 22.02           ~ 1 0
29 ACO 267 ClG 01 52 43.016 +00 59 58.90           ~ 241 0
30 ACO 370 ClG 02 39 50.5 -01 35 08           ~ 825 0
31 [KBB2019] ACT-CL J0239.8-0134 G Rad 02 39 50.78 -01 35 42.7           ~ 1 0
32 [KBB2019] ACT-CL J0239.8-0134 H Rad 02 39 51.90 -01 35 58.8           ~ 1 0
33 SDSS J023952.72-013418.8 rG 02 39 52.732 -01 34 18.90   23.070     19.826 ~ 26 0
34 [KBB2019] ACT-CL J0239.8-0134 E Rad 02 39 52.96 -01 35 00.6           ~ 1 0
35 CN A370 94 rG 02 39 54.1881 -01 35 08.925   23.186     19.926 ~ 14 0
36 BOW ACO 370 CC039 rG 02 39 54.440 -01 33 36.03   20.13       ~ 12 1
37 SDSS J023955.32-013405.7 rG 02 39 55.3212 -01 34 05.736   23.217     19.940 ~ 16 0
38 [KBB2019] ACT-CL J0239.8-0134 C Rad 02 39 56.37 -01 34 29.4           ~ 1 0
39 NGC 1143 IG 02 55 09.7142741256 -00 10 40.248085584   13.2       ~ 154 1
40 [KBB2019] ACT-CL J0256.5+0006 E Rad 02 56 27.830 +00 06 50.70           ~ 1 0
41 [KBB2019] ACT-CL J0256.5+0006 F Rad 02 56 28.982 +00 06 30.50           ~ 1 0
42 SDSS J025630.84+000603.2 rG 02 56 30.849 +00 06 03.26           ~ 8 0
43 [KIB2016] S6 Rad 02 56 32.20 +00 05 50.8           ~ 2 0
44 [KIB2016] S4 Rad 02 56 32.60 +00 06 30.9           ~ 2 0
45 ClG J0256+0006 ClG 02 56 32.9 +00 06 12           ~ 42 0
46 SDSS J025633.76+000628.7 rG 02 56 33.767 +00 06 28.76           ~ 6 0
47 NVSS J025633+000502 rG 02 56 33.88961 +00 05 01.9255           ~ 5 0
48 [KBB2019] ACT-CL J0256.5+0006 RH Rad 02 56 34.328 +00 05 59.67           ~ 1 0
49 SDSS J025635.53+000610.7 rG 02 56 35.5352 +00 06 10.703           ~ 5 0
50 [KIB2016] S2 Rad 02 56 35.90 +00 06 27.9           ~ 2 0
51 ACO 1958 ClG 14 43 13 +30 58.3           ~ 53 0
52 ACO 2146 ClG 15 56 04.7 +66 20 24           ~ 192 0
53 [KBB2019] ACT-CL J2051.1+0215 D Rad 20 51 04.866 +02 17 01.03           ~ 1 0
54 [KBB2019] ACT-CL J2051.1+0215 F Rad 20 51 04.920 +02 14 47.67           ~ 1 0
55 [KBB2019] ACT-CL J2051.1+0215 C Rad 20 51 10.310 +02 17 12.57           ~ 1 0
56 [KBB2019] ACT-CL J2051.1+0215 B Rad 20 51 11.370 +02 16 45.36           ~ 1 0
57 ACT-CL J2051.1+0215 ClG 20 51 12.20 +02 15 58.3           ~ 23 0
58 [KBB2019] ACT-CL J2051.1+0215 A Rad 20 51 15.650 +02 16 06.03           ~ 1 0
59 ClG J2129+0005 ClG 21 29 40.5 +00 05 47           ~ 308 0
60 [KBB2019] ACT-CL J2135.2+0125 B Rad 21 35 15.619 +01 24 50.15           ~ 1 0
61 ACO 2355 ClG 21 35 18.70 +01 25 27.0           ~ 75 0
62 LEDA 1194484 rG 21 35 18.7717201344 +01 25 27.029560368   19.4       ~ 10 0
63 ACT-CL J2135.7+0009 ClG 21 35 39.50 +00 09 57.1           ~ 5 0
64 ACO 2356 ClG 21 35 45.13 +00 11 21.1           ~ 46 0
65 ACT-CL J2154.5-0049 ClG 21 54 32.30 -00 49 00.4           ~ 13 0
66 [KBB2019] ACT-CL J2154.5-0049 B Rad 21 54 32.532 -00 49 55.02           ~ 1 0
67 SDSS J215436.04-004952.0 Rad 21 54 36.049 -00 49 52.10           ~ 2 0
68 ICRF J232653.7-020213 BLL 23 26 53.77670595 -02 02 13.7811657   18.3       ~ 60 1
69 ACT-CL J2327.4-0204 ClG 23 27 27.60 -02 04 37.4           ~ 44 0
70 SDSS J233739.73+001616.9 rG 23 37 39.756 +00 16 16.51   19.6       ~ 21 0
71 [KBB2019] ACT-CL J2337.6+0016 A Rad 23 37 40.657 +00 16 49.87           ~ 1 0
72 ACO 2631 ClG 23 37 40.7 +00 16 35           ~ 183 0
73 [KBB2019] ACT-CL J2337.6+0016 C Rad 23 37 43.437 +00 17 03.30           ~ 1 0
74 [KBB2019] ACT-CL J2337.6+0016 B Rad 23 37 44.473 +00 17 28.61           ~ 1 0
75 ACT-CL J2344.7-4243 ClG 23 44 43.9 -42 43 11           ~ 229 0

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