2011MNRAS.413.2121M


Query : 2011MNRAS.413.2121M

2011MNRAS.413.2121M - Mon. Not. R. Astron. Soc., 413, 2121-2139 (2011/May-3)

Cusped mass density profiles and magnification ratios of double-image gravitational lenses.

MUTKA P.T.

Abstract (from CDS):

We have been able to connect statistics of the observed double-image gravitational lenses to general properties of the internal structure of lens haloes. Our analytical theory for the generalization of the Navarro, Frenk & White (NFW) profile (GNFW) lenses with a parametrized cusp slope (α) gives a relation connecting the cusp slope of a lens mass profile to the observed magnification ratio of the produced images and location of the optical axis. The relation does not depend on the cosmology, total lens mass, concentration or redshifts of the the lens and the lensed object. Simple geometry of axially-symmetric lensing and the aforementioned relation enables us to define the cusp slope limit value, αCSL, for the cusp slope, independent of the location of the optical axis. The threshold cusp slope value α=αCSL is the shallowest slope for the inner part of the GNFW profile that can produce the observed magnification ratio with any lensing configuration. We use a distribution of these threshold values that depend only on the observed flux ratio of the lensed images, in a statistical study of the double image lenses in order to limit the possible cusp slope values and identify whether there exists a population of haloes with similar profiles. Our theoretical fit indicates that within our sample of double-image gravitational lenses, most of the haloes have the cusp slope α=-1.95±0.02. We have also found an indication of a second population of lenses with a cusp slope value α=-1.51 ±0.02. We estimate that there is about 97 per cent probability that the observed feature in the threshold value limit distribution is produced by a second population of lenses, with their own characteristic density profile. The data indicating the exact characteristics of the subpopulation are noisy. Roughly one out of eight haloes within the sample belongs to this shallower cusp slope group. We investigate the accuracy of our analysis by constructing mock catalogues with Monte Carlo method. The He-rich stripped-envelope core-collapse supernova 2008ax

Abstract Copyright: 2011 The Author Monthly Notices of the Royal Astronomical Society2011 RAS

Journal keyword(s): gravitational lensing: strong - methods: analytical - galaxies: haloes - dark matter

Simbad objects: 44

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Number of rows : 44
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 [WSC2004] HE 0047-1756 gLS 00 50 27.83 -17 40 11.2           ~ 6 0
2 QSO B0142-100 QSO 01 45 16.5958283760 -09 45 17.265131352   17.23 16.95     ~ 247 1
3 QSO J0158-4325 QSO 01 58 41.3988 -43 25 03.798   17.2 17.2     ~ 74 1
4 [IBG2005] SDSS J0246-0825 gLS 02 46 34.09 -08 25 35.9           ~ 10 0
5 CLASS B0445+123 rG 04 48 +12.4           ~ 24 0
6 QSO B0512-3329 QSO 05 14 10.91 -33 26 22.4     17.0     ~ 62 0
7 CLASS B0631+519 rG 06 35 +51.9           ~ 22 0
8 CLASS B0739+366 LeQ 07 42 51 +36 34.7           ~ 18 0
9 QSO J0746+4403 QSO 07 46 53.0413 +44 03 51.464   19.29 19.12     ~ 25 0
10 [VV2006] J082139.1+121729 QSO 08 21 38.9423240760 +12 17 29.991158088   19.23 18.99     ~ 53 1
11 [VV2006] J083105.4+522520 QSO 08 31 05.413 +52 25 20.60     19.60     ~ 14 3
12 CLASS B0850+054 rG 08 53 +05.2           ~ 25 0
13 [VV2006] J090334.9+502819 QSO 09 03 34.9475 +50 28 19.293   22.90 21.49     ~ 44 2
14 QSO B0909+5312 QSO 09 13 01.031 +52 59 28.90   17.29 16.71     ~ 157 1
15 [VV2006] J092112.8+452905 QSO 09 21 12.8304560016 +45 29 03.987252096   19.09 18.71     ~ 38 2
16 [VV98] J095122.6+263513 QSO 09 51 22.5840 +26 35 13.786   17.66 17.31     ~ 120 1
17 QSO B0952-0115 QSO 09 55 00.1037541106 -01 30 06.549307797     18.7     ~ 150 0
18 8C 0958+561 QSO 10 01 20.6918953728 +55 53 55.593949272   17.16 16.95     ~ 757 3
19 [OIH2005] SDSS J1001+5027 gLS 10 01 28.6 +50 27 57           ~ 19 0
20 QSO J1004+1229 QSO 10 04 24.8871 +12 29 22.245   24.83 23.23 20.80   ~ 53 1
21 LBQS 1009-0252 QSO 10 12 15.89 -03 07 03.1   18.82 18.71     ~ 75 1
22 QSO B1015-205 QSO 10 17 23.98 -20 46 58.6   17.08 17.08     ~ 71 2
23 [VV2006] J102111.0+491330 QSO 10 21 11.0253 +49 13 30.344   19.49 19.33     ~ 30 1
24 QSO B1030+074 Bla 10 33 34.02429368 +07 11 26.1475933     20.34 20.22   ~ 111 2
25 QSO B1104-181 QSO 11 06 33.3845199936 -18 21 23.829049296   15.8 15.9 15.7   ~ 338 1
26 NVSS J113000+381203 Rad 11 30 00.110 +38 12 03.23           ~ 31 0
27 [PEI2004] SDSS J1155+6346 gLS 11 55 17.3 +63 46 22           ~ 13 0
28 [VV2000] J115518.3+193942 QSO 11 55 18.2955044232 +19 39 42.228456840   17.15 16.89     ~ 100 2
29 [OIH2005] SDSS J1206+4332 gLS 12 06 29.6 +43 32 17           ~ 63 0
30 QSO B1208+101 QSO 12 10 57.0369007056 +09 54 27.069784092     17.5     ~ 113 1
31 [ECM2006] SDSS J1226-0006 gLS 12 26 08.020 -00 06 02.19           ~ 10 0
32 LBQS 1333+0133 QSO 13 35 34.7884118928 +01 18 05.531756724   18.39 18.17     ~ 62 2
33 QSO B1352-2242 QSO 13 55 43.4224 -22 57 23.388   18.2 18.2     ~ 37 1
34 QSO B1520+530 QSO 15 21 44.8 +52 54 49   18.2       ~ 123 2
35 QSO B1600+4344 QSO 16 01 40.4818 +43 16 47.394   22.12 21.92     ~ 188 1
36 [VV2006] J163257.6-003302 Bla 16 32 57.68123332 -00 33 21.0701388     20.99 20   ~ 60 2
37 [VV2000] J163348.9+313411 QSO 16 33 48.9842 +31 34 11.871   17.1 17.41 17.0   ~ 58 1
38 QSO J1650+4251 QSO 16 50 43.4447423448 +42 51 49.367524032   17.78 17.58     ~ 67 1
39 QSO B1830-211 Bla 18 33 39.9399138048 -21 03 39.368838780     18.70 21   ~ 724 1
40 [VV2006] J183828.7-342733 QSO 18 38 28.4967892128 -34 27 41.764115592     19.21     ~ 43 2
41 PMN J2004-1349 QSO 20 04 07.09 -13 49 31.1           ~ 22 1
42 NVSS J211054+213059 Rad 21 10 54.06 +21 30 58.7           ~ 30 1
43 FIRST J232140.7+052737 Rad 23 21 40.801 +05 27 37.23           ~ 29 1

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