2019ApJ...872...11H


Query : 2019ApJ...872...11H

2019ApJ...872...11H - Astrophys. J., 872, 11-11 (2019/February-2)

Strong gravitational lensing by wave dark matter halos.

HERRERA-MARTIN A., HENDRY M., GONZALEZ-MORALES A.X. and URENA-LOPEZ L.A.

Abstract (from CDS):

Wave dark matter (WaveDM) has recently gained attention as a viable candidate to account for the dark matter content of the universe. In this paper we explore the extent to which, and under what conditions, dark matter halos in this model are able to reproduce strong-lensing systems. First, we explore analytically the lensing properties of the model, finding that a pure WaveDM density profile, the soliton profile, produces a weaker lensing effect than similar cored profiles. Then, we analyze models with a soliton embedded within a Navarro, Frenk, and White (NFW) profile, as has been found in numerical simulations of structure formation. We use a benchmark model with a boson mass of ma = 10–22 eV, for which we see that there is a bimodality in the contribution of the external NFW part of the profile, and some of the free parameters associated with it are not well constrained. We find that for configurations with boson masses 10–23 to 10–22 eV, a range of masses preferred by dwarf galaxy kinematics, the soliton profile alone can fit the data, but its size is incompatible with the luminous extent of the lens galaxies. Likewise, boson masses of the order of 10–21 eV, which would be consistent with Lyα constraints and consist of more compact soliton configurations, necessarily require the NFW part in order to reproduce the observed Einstein radii. We then conclude that lens systems impose a conservative lower bound ma > 10–24 eV and that the NFW envelope around the soliton must be present to satisfy the observational requirements.

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

Journal keyword(s): dark matter - Galaxy: halo - gravitational lensing: strong

Simbad objects: 25

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Number of rows : 25
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 SLACS SDSS J0008-0004 gLS 00 08 02.953 -00 04 08.21           ~ 17 0
2 SDSS J000802.95-000408.2 G 00 08 02.953 -00 04 08.21     19.60   18.65 ~ 6 0
3 SLACS SDSS J0008-0004 source LeG 00 08 02.96 -00 04 08.2           ~ 4 0
4 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 12678 1
5 CFRS 03.1077 G 03 02 32.59 +00 06 00.0           ~ 25 1
6 [CSH2002] Lensed G G 03 02 33.0 +00 06 00           ~ 7 1
7 SLACS SDSS J0935-0003 source LeG 09 35 43.93 -00 03 34.8           ~ 10 1
8 SLACS SDSS J0935-0003 gLS 09 35 43.933 -00 03 34.78           ~ 22 0
9 SLACS SDSS J0935-0003 lens BiC 09 35 43.933 -00 03 34.78   19.36 17.71   16.75 ~ 16 1
10 SLACS SDSS J0946+1006 source LeG 09 46 56.6809160256 +10 06 52.903093212           ~ 9 0
11 SDSS J094656.68+100652.8 G 09 46 56.6809160256 +10 06 52.903093212     17.78   17.09 ~ 31 0
12 SLACS SDSS J0946+1006 gLS 09 46 56.6809160256 +10 06 52.903093212           ~ 52 0
13 SLACS SDSS J1143-0144 gLS 11 43 29.6380595424 -01 44 29.975242920           ~ 29 0
14 6dFGS gJ114329.6-014430 BiC 11 43 29.6380595424 -01 44 29.975242920   17.21 15.83 15.81 14.96 ~ 23 0
15 LEDA 139673 LeG 11 43 29.6380595424 -01 44 29.975242920           ~ 9 0
16 SLACS SDSS J1306+0600 source G 13 06 13.6521551928 +06 00 22.112577792           ~ 3 1
17 SLACS SDSS J1306+0600 gLS 13 06 13.6521551928 +06 00 22.112577792           ~ 8 0
18 SDSS J130613.65+060022.1 G 13 06 13.6521551928 +06 00 22.112577792   18.83 17.91   16.76 ~ 7 1
19 SLACS SDSS J1318-0313 source G 13 18 39.3260056512 -03 13 34.304732220           ~ 2 0
20 SDSS J131839.32-031334.2 BiC 13 18 39.3260056512 -03 13 34.304732220     17.54   16.80 ~ 8 0
21 SLACS SDSS J1318-0313 gLS 13 18 39.3260056512 -03 13 34.304732220           ~ 7 0
22 CFRS 14.1311 G 14 17 35.70 +52 26 45.9   24.04 21.53 21.38 19.971 ~ 62 1
23 QSO J1417+5226 QSO 14 17 35.738 +52 26 46.34           ~ 21 0
24 SL2S J220329+020518 source G 22 03 29.0 +02 05 19           ~ 3 0
25 SL2S J220329+020518 gLe 22 03 29.030 +02 05 18.89           ~ 14 0

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