2019MNRAS.482.1043C

Query : 2019MNRAS.482.1043C

2019MNRAS.482.1043C - Mon. Not. R. Astron. Soc., 482, 1043-1061 (2019/January-1)

Galaxy kinematics and mass calibration in massive SZE-selected galaxy clusters to z = 1.3.

CAPASSO R., SARO A., MOHR J.J., BIVIANO A., BOCQUET S., STRAZZULLO V., GRANDIS S., APPLEGATE D.E., BAYLISS M.B., BENSON B.A., BLEEM L.E., BRODWIN M., BULBUL E., CARLSTROM J.E., CHIU I., DIETRICH J.P., GUPTA N., DE HAAN T., HLAVACEK-LARRONDO J., KLEIN M., VON DER LINDEN A., McDONALD M., RAPETTI D., REICHARDT C.L., SHARON K., STALDER B., STANFORD S.A., STARK A.A., STERN C. and ZENTENO A.

Abstract (from CDS):

The galaxy phase-space distribution in galaxy clusters provides insights into the formation and evolution of cluster galaxies, and it can also be used to measure cluster mass profiles. We present a dynamical study based on ∼3000 passive, non-emission-line cluster galaxies drawn from 110 galaxy clusters. The galaxy clusters were selected using the Sunyaev-Zel'dovich effect (SZE) in the 2500 deg2 South Pole Telescope (SPT)-SZ survey and cover the redshift range 0.2 < z < 1.3. We model the clusters using the Jeans equation, while adopting NFW mass profiles and a broad range of velocity dispersion anisotropy profiles. The data prefer velocity dispersion anisotropy profiles that are approximately isotropic near the centre and increasingly radial toward the cluster virial radius, and this is true for all redshifts and masses we study. The pseudo-phase-space density profile of the passive galaxies is consistent with expectations for dark matter particles and subhaloes from cosmological N-body simulations. The dynamical mass constraints are in good agreement with external mass estimates of the SPT cluster sample from either weak lensing, velocity dispersions, or X-ray YX measurements. However, the dynamical masses are lower (at the 2.2σ level) when compared to the mass calibration favoured when fitting the SPT cluster data to a Λcold dark matter model with external cosmological priors, including cosmic microwave background anisotropy data from Planck. The discrepancy grows with redshift, where in the highest redshift bin the ratio of dynamical to SPT + Planck masses is η= 0.63+0.13–0.08±0.06 (statistical and systematic), corresponding to a 2.6σ discrepancy.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): galaxies: clusters: general - galaxies: evolution - galaxies: kinematics and dynamics - galaxies: statistics - cosmology: observations - large-scale structure of Universe

Simbad objects: 112

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Number of rows : 112
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 ACT-CL J0000.9-5748 ClG 00 01 00 -57 48.5           ~ 57 0
2 ACT-CL J0013.3-4906 ClG 00 13 19.315 -49 06 37.78           ~ 28 0
3 ACT-CL J0014.8-4952 ClG 00 14 48.2896 -49 52 30.837           ~ 28 0
4 PSZ2 G306.22-53.56 ClG 00 33 53 -63 26.6           ~ 25 0
5 ACT-CL J0037.7-5047 ClG 00 37 45.7107 -50 47 30.138           ~ 22 0
6 ACT-CL J0040.8-4407 ClG 00 40 49.9 -44 07 50           ~ 43 0
7 ACO 85 ClG 00 41 36.21 -09 19 30.4           ~ 974 0
8 ACT-CL J0102.6-4603 ClG 01 02 40.9347 -46 03 48.237           ~ 24 0
9 ACT-CL J0102-4915 ClG 01 02 52.50 -49 14 58.0           ~ 296 0
10 ACT-CL J0106.4-5942 ClG 01 06 28.737 -59 43 12.54           ~ 25 0
11 ACT-CL J0118.3-5156 ClG 01 18 20.3322 -51 56 16.527           ~ 13 0
12 ACT-CL J0123.1-4821 ClG 01 23 09.3334 -48 21 28.638           ~ 25 0
13 ACT-CL J0142.1-5032 ClG 01 42 10.9175 -50 32 28.944           ~ 21 0
14 ACT-CL J0200.5-4852 ClG 02 00 34 -48 52.3           ~ 25 0
15 SPT-CL J0205-6432 ClG 02 05 06.9 -64 32 46           ~ 11 0
16 ACT-CL J0205.7-5829 ClG 02 05 46.5 -58 29 08           ~ 54 0
17 ACT-CL J0212.4-4656 ClG 02 12 26 -46 57.0           ~ 24 0
18 ACT-CL J0232-5257 ClG 02 32 42.709 -52 57 22.61           ~ 33 0
19 ACT-CL J0233.0-5819 ClG 02 33 00.9 -58 19 38           ~ 19 0
20 ACT-CL J0234.7-5831 ClG 02 34 43.4 -58 31 25           ~ 40 0
21 ACT-CL J0235.7-5120 ClG 02 35 45.30 -51 21 05.2           ~ 42 0
22 ACT-CL J0236.9-4937 ClG 02 36 58.8749 -49 37 45.991           ~ 27 0
23 ACT-CL J0240.6-5946 ClG 02 40 37.9915 -59 46 00.417           ~ 20 0
24 ACT-CL J0243.4-5931 ClG 02 43 28 -59 30.9           ~ 26 0
25 ACT-CL J0243.5-4833 ClG 02 43 38.873 -48 33 38.94           ~ 26 0
26 ACT-CL J0252.7-4824 ClG 02 52 45.8600 -48 24 43.327           ~ 22 0
27 ACT-CL J0254.3-5857 ClG 02 54 17.7 -58 57 11           ~ 57 0
28 SPT-CL J0257-5732 ClG 02 57 21.5 -57 32 53           ~ 15 0
29 ACT-CL J0304.2-4921 ClG 03 04 14.6510 -49 21 27.364           ~ 37 0
30 ACT-CL J0304.2-4401 ClG 03 04 20.29 -44 02 27.8           ~ 41 0
31 PSZSPT J0307-6225 ClG 03 07 19 -62 26.2           ~ 30 0
32 ACT-CL J0310.5-4647 ClG 03 10 32.7023 -46 47 02.198           ~ 23 0
33 ACT-CL J0317.2-5935 ClG 03 17 15.6160 -59 35 10.664           ~ 21 0
34 MARD J032414.5-623537 ClG 03 24 12.240 -62 35 55.80           ~ 27 0
35 ACT-CL J0330.9-5228 ClG 03 30 56.3 -52 28 19           ~ 53 0
36 ACT-CL J0334.2-4659 ClG 03 34 11.180 -46 59 39.50           ~ 27 0
37 ACT-CL J0346.9-5438 ClG 03 46 55.50 -54 38 54.8           ~ 33 0
38 ClG 0346-45 ClG 03 48 17.560 -45 15 01.06           ~ 32 0
39 ACT-CL J0352.9-5647 ClG 03 52 57.7496 -56 47 52.643           ~ 27 0
40 ACT-CL J0356.3-5337 ClG 03 56 19.6560 -53 37 45.752           ~ 16 0
41 ACT-CL J0403.8-5719 ClG 04 03 52.1 -57 19 43           ~ 19 0
42 ACT-CL J0406.8-4804 ClG 04 06 55 -48 04.9           ~ 25 0
43 ACT-CL J0411.2-4819 ClG 04 11 15.321 -48 19 20.49           ~ 41 0
44 ACT-CL J0417.3-4748 ClG 04 17 21.3437 -47 48 46.370           ~ 37 0
45 ACT-CL J0426.0-5455 ClG 04 26 02.7598 -54 55 09.371           ~ 28 0
46 ACT-CL J0432.9-5630 ClG 04 33 00.5 -56 30 14           ~ 15 0
47 ACT-CL J0438.2-5419 ClG 04 38 17.70 -54 19 20.7           ~ 78 0
48 ACT-CL J0449.0-4901 ClG 04 49 04.8508 -49 01 28.759           ~ 29 0
49 ACT-CL J0456.4-5116 ClG 04 56 28.1 -51 16 35           ~ 31 0
50 ACT-CL J0509.3-5342 ClG 05 09 21.40 -53 42 12.3           ~ 62 0
51 ACT-CL J0511.6-5154 ClG 05 11 41.31 -51 54 20.8           ~ 22 0
52 ACO S 520 ClG 05 16 37.40 -54 30 01.5           ~ 114 0
53 ACT-CL J0521.2-5104 ClG 05 21 12.6431 -51 04 18.700           ~ 21 0
54 ACT-CL J0528-5259 ClG 05 28 05.30 -52 59 52.8           ~ 52 0
55 SPT-CL J0533-5005 ClG 05 33 37 -50 05.8           ~ 37 0
56 SPT-CL J0534-5937 ClG 05 34 24.4 -59 37 44           ~ 11 0
57 ACT-CL J0539.9-5744 ClG 05 39 59.538 -57 44 37.28           ~ 20 0
58 ClG J0542-4100 ClG 05 42 49.9 -40 59 58           ~ 67 0
59 ACT-CL J0546.6-5345 ClG 05 46 37.6557 -53 45 33.242           ~ 98 0
60 PLCKESZ G271.2-31.0 ClG 05 49 16 -62 05.2           ~ 41 0
61 ACT-CL J0551.6-5709 ClG 05 51 36.000 -57 09 22.00           ~ 37 0
62 PSZ1 G273.55-30.28 ClG 05 55 24.4 -64 06 47           ~ 26 0
63 ACT-CL J0559.7-5249 ClG 05 59 43.20 -52 49 27.1           ~ 63 0
64 ACT-CL J0655.8-5234 ClG 06 55 53.8293 -52 34 31.654           ~ 22 0
65 PSZSPT J2017-6258 ClG 20 17 55.9 -62 58 32           ~ 13 0
66 SPT-CL J2020-6314 ClG 20 20 07.2 -63 14 29           ~ 11 0
67 PSZSPT J2022-6324 ClG 20 22 05.6 -63 23 50           ~ 20 0
68 SPT-CL J2026-4513 ClG 20 26 27.4 -45 13 32           ~ 9 0
69 ACT-CL J2030.8-5638 ClG 20 30 49.6 -56 38 07           ~ 20 0
70 ACO 3685 ClG 20 32 19.2 -56 27 21           ~ 46 0
71 ACT-CL J2035.1-5251 ClG 20 35 10.9847 -52 51 11.438           ~ 23 0
72 ACT-CL J2040.2-5725 ClG 20 40 13.2 -57 25 18           ~ 19 0
73 ACT-CL J2043.2-5035 ClG 20 43 16.7205 -50 35 30.861           ~ 47 0
74 ACT-CL J2056.8-5459 ClG 20 56 54.0 -54 59 13           ~ 17 0
75 ACT-CL J2058.3-5608 ClG 20 58 21.0053 -56 08 30.000           ~ 13 0
76 SPT-CL J2100-4548 ClG 21 00 22.5 -45 48 21           ~ 10 0
77 ACT-CL J2106.0-5844 ClG 21 06 04.3 -58 44 32           ~ 103 0
78 SPT-CL J2115-4659 ClG 21 15 11.9 -46 59 10           ~ 8 0
79 PSZSPT J2119-5055 ClG 21 18 55.0 -50 55 58           ~ 12 0
80 1eRASS J212433.5-612500 ClG 21 24 35.3 -61 24 42           ~ 15 0
81 MARD J213049.6-645946 ClG 21 30 56.209 -64 58 40.32           ~ 16 0
82 ACT-CL J2135.6-5726 ClG 21 35 39.8 -57 26 29           ~ 30 0
83 MARD J213622.8-470520 ClG 21 36 27.862 -47 05 06.99           ~ 12 0
84 PSZSPT J2136-6307 ClG 21 36 56.0 -63 07 24           ~ 13 0
85 1eRASS J213800.9-600758 ClG 21 38 00.059 -60 07 54.34           ~ 25 0
86 SPT-CL J2140-5727 ClG 21 40 33.1 -57 27 23           ~ 10 0
87 ACT-CL J2145.8-5645 ClG 21 45 51.8 -56 44 49           ~ 30 0
88 PSZSPT J2146-4846 ClG 21 46 08.3 -48 46 39           ~ 12 0
89 ACT-CL J2146.5-4633 ClG 21 46 34.8 -46 32 56           ~ 36 0
90 ACT-CL J2146.8-5736 ClG 21 46 48.942 -57 36 49.57           ~ 16 0
91 PSZ1 G331.63-44.33 ClG 21 48 49.7 -61 17 03           ~ 27 0
92 SPT-CL J2155-6048 ClG 21 55 56.4 -60 48 26           ~ 11 0
93 PSZSPT J2159-6244 ClG 21 59 58.1 -62 44 31           ~ 12 0
94 ACT-CL J2222.8-4834 ClG 22 22 50.682 -48 34 35.12           ~ 27 0
95 ACT-CL J2232.5-5959 ClG 22 32 33.1423 -59 59 13.374           ~ 24 0
96 ACT-CL J2233.3-5338 ClG 22 33 17 -53 39.2           ~ 24 0
97 ACO S 1063 ClG 22 48 45.4 -44 31 42           ~ 395 0
98 SUMSS J230039-533116 Bla 23 00 39.7245361488 -53 31 11.890928136           ~ 18 0
99 ACO S 1079 ClG 23 00 41.8 -53 31 28           ~ 21 0
100 SPT-CL J2301-5546 ClG 23 01 53 -55 46.6           ~ 16 0
101 PSZ1 G319.20-48.61 ClG 23 07 00.9156 -65 06 03.268           ~ 25 0
102 ACO S 1121 ClG 23 25 12.2988 -41 11 45.461           ~ 46 0
103 PSZSPT J2331-5052 ClG 23 31 51 -50 51.9           ~ 53 0
104 ACT-CL J2332.4-5358 ClG 23 32 26.70 -53 58 20.4           ~ 52 0
105 ACT-CL J2335.1-4544 ClG 23 35 07.7929 -45 44 18.347           ~ 30 0
106 ACT-CL J2337.4-5942 ClG 23 37 24.2 -59 42 17           ~ 52 0
107 ACT-CL J2341.2-5119 ClG 23 41 12.3 -51 19 43           ~ 52 0
108 ACT-CL J2342.7-5411 ClG 23 42 45.6153 -54 11 11.527           ~ 44 0
109 ACT-CL J2344.7-4243 ClG 23 44 43.9 -42 43 11           ~ 229 0
110 ACT-CL J2351.6-5452 ClG 23 51 36.4073 -54 52 51.379           ~ 20 0
111 ACT-CL J2355.7-5055 ClG 23 55 49.000 -50 56 13.00           ~ 37 0
112 ACT-CL J2359.7-5010 ClG 23 59 44 -50 10.2           ~ 38 0

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