2014ApJ...794..136D


Query : 2014ApJ...794..136D

2014ApJ...794..136D - Astrophys. J., 794, 136 (2014/October-3)

CLASH-x: a comparison of lensing and X-ray techniques for measuring the mass profiles of galaxy clusters.

DONAHUE M., VOIT G.M., MAHDAVI A., UMETSU K., ETTORI S., MERTEN J., POSTMAN M., HOFFER A., BALDI A., COE D., CZAKON N., BARTELMANN M., BENITEZ N., BOUWENS R., BRADLEY L., BROADHURST T., FORD H., GASTALDELLO F., GRILLO C., INFANTE L., JOUVEL S., KOEKEMOER A., KELSON D., LAHAV O., LEMZE D., MEDEZINSKI E., MELCHIOR P., MENEGHETTI M., MOLINO A., MOUSTAKAS J., MOUSTAKAS L.A., NONINO M., ROSATI P., SAYERS J., SEITZ S., VAN DER WEL A., ZHENG W. and ZITRIN A.

Abstract (from CDS):

We present profiles of temperature, gas mass, and hydrostatic mass estimated from new and archival X-ray observations of CLASH clusters. We compare measurements derived from XMM and Chandra observations with one another and compare both to gravitational lensing mass profiles derived with CLASH Hubble Space Telescope and Subaru Telescope lensing data. Radial profiles of Chandra and XMM measurements of electron density and enclosed gas mass are nearly identical, indicating that differences in hydrostatic masses inferred from X-ray observations arise from differences in gas-temperature measurements. Encouragingly, gas temperatures measured in clusters by XMM and Chandra are consistent with one another at ∼100-200 kpc radii, but XMM temperatures systematically decline relative to Chandra temperatures at larger radii. The angular dependence of the discrepancy suggests that additional investigation on systematics such as the XMM point-spread function correction, vignetting, and off-axis responses is yet required. We present the CLASH-X mass-profile comparisons in the form of cosmology-independent and redshift-independent circular-velocity profiles. We argue that comparisons of circular-velocity profiles are the most robust way to assess mass bias. Ratios of Chandra hydrostatic equilibrium (HSE) mass profiles to CLASH lensing profiles show no obvious radial dependence in the 0.3-0.8 Mpc range. However, the mean mass biases inferred from the weak-lensing (WL) and SaWLens data are different. As an example, the weighted-mean value at 0.5 Mpc is < b > = 0.12 for the WL comparison and < b > = -0.11 for the SaWLens comparison. The ratios of XMM HSE mass profiles to CLASH lensing profiles show a pronounced radial dependence in the 0.3-1.0 Mpc range, with a weighted mean mass bias value rising to < b > ≳ 0.3 at ∼1 Mpc for the WL comparison and < b > ~ 0.25 for the SaWLens comparison. The enclosed gas mass profiles from both Chandra and XMM rise to a value ~1/8 times the total-mass profiles inferred from lensing at ~0.5 Mpc and remain constant outside of that radius, suggesting that Mgasx8 profiles may be an excellent proxy for total-mass profiles at ≳ 0.5 Mpc in massive galaxy clusters.

Abstract Copyright: ∼

Journal keyword(s): cosmological parameters - dark matter - galaxies: clusters: intracluster medium - gravitational lensing: strong - gravitational lensing: weak - X-rays: galaxies: clusters

Simbad objects: 27

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Number of rows : 27
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 ACO 209 ClG 01 31 52.9 -13 36 53           ~ 326 0
2 ACO 383 ClG 02 48 03.3915 -03 31 45.228           ~ 389 0
3 RX J0329.6-0211 ClG 03 29 41.6 -02 11 47           ~ 155 0
4 MCS J0416.1-2403 ClG 04 16 08.380 -24 04 20.80           ~ 425 0
5 ClG J0429-0253 ClG 04 29 36.0 -02 53 09           ~ 131 0
6 ClG J0647+7015 ClG 06 47 50.0 +70 14 55           ~ 177 0
7 ClG J0717+3745 ClG 07 17 36.50 +37 45 23.0           ~ 511 0
8 B3 0714+378 Rad 07 17 36.6 +37 45 01           ~ 170 2
9 ClG J0744+3927 ClG 07 44 52.5 +39 27 30           ~ 189 0
10 ACO 611 ClG 08 00 58.7 +36 02 49           ~ 275 0
11 MCS J1115.8+0129 ClG 11 15 52.1 +01 29 53           ~ 142 0
12 MCS J1149.5+2223 ClG 11 49 35.8 +22 23 55           ~ 546 0
13 ACO 1423 ClG 11 57 17.3206 +33 36 39.364           ~ 181 0
14 MCS J1206.2-0847 ClG 12 06 12.2 -08 48 02           ~ 286 0
15 ClG J1226+3332 ClG 12 26 57.7 +33 32 50           ~ 228 0
16 ClG J1311-0311 ClG 13 11 01.7 -03 10 38           ~ 120 0
17 ClG J1347-1145 ClG 13 47 30.5 -11 45 07           ~ 577 0
18 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 727 1
19 ClG J1423+2404 ClG 14 23 47.7 +24 04 40           ~ 231 0
20 ClG J1532+3021 ClG 15 32 53.8 +30 21 00           ~ 122 0
21 ClG J1720+3536 ClG 17 20 16.8 +35 36 27           ~ 150 1
22 ACO 2261 ClG 17 22 26.9 +32 07 58           ~ 370 0
23 ClG J1931-2635 ClG 19 31 49.6 -26 34 33           ~ 181 0
24 ClG J2129-0741 ClG 21 29 26.0 -07 41 28           ~ 189 0
25 ClG J2129+0005 ClG 21 29 40.5 +00 05 47           ~ 308 0
26 ClG 2137-2353 ClG 21 40 12.8 -23 39 27     18.5     ~ 390 0
27 ACO S 1063 ClG 22 48 45.4 -44 31 42           ~ 395 0

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