TY - JOUR
T1 - Strong lensing in Abell 1703: constraints on the slope of the inner dark matter distribution
AU - Limousin, M.
AU - Richard, J.
AU - Kneib, J.-P.
AU - Brink, H.
AU - Pelló, R.
AU - Jullo, E.
AU - Tu, H.
AU - Sommer-Larsen, J.
AU - Egami, E.
AU - Michalowski, Michal
AU - Cabanac, R.
AU - Stark, D. P.
PY - 2008/10/1
Y1 - 2008/10/1
N2 - Properties of dark matter haloes can be probed observationally and
numerically, and comparing both approaches provides ways to constrain
cosmological models. When it comes to the inner part of galaxy cluster
scale haloes, interaction between the baryonic and the dark matter
component is an important issue that is far from being fully understood.
With this work, we aim to initiate a program coupling observational and
numerical studies to probe the inner part of galaxy clusters. In this
article, we apply strong lensing techniques on Abell 1703, a massive
X-ray luminous galaxy cluster at z = 0.28. Our analysis is based on
imaging data from both the space and ground in 8 bands, complemented by
a spectroscopic survey. Abell 1703 is rather circular from the general
shape of its multiply imaged systems and is dominated by a giant
elliptical cD galaxy in its centre. This cluster exhibits a remarkable
bright central ring formed by 4 images at z_spec = 0.888 only 5-13
arcsec away from the cD centre. This unique feature offers a rare
lensing constrain for probing the central mass distribution. The stellar
contribution from the cD galaxy (˜1.25 × 1012
Msun within 30 kpc) is accounted for in our parametric mass
modelling, and the underlying smooth dark matter component distribution
is described using a generalized nfw profile parametrized with a central
logarithmic slope α. The rms of our mass model in the image plane
is equal to 1.4 arcsec. We find that within the range where
observational constraints are present (from 20 kpc to 210 kpc),
α is equal to 1.09+0.05-0.11 (3σ
confidence level). The concentration parameter is equal to
c200 3.5, and the scale radius is constrained to be larger
than the region where observational constraints are available
(rs =730^+15-75 kpc). The 2D mass is equal to {M}
(210 kpc) = 2.4 × 1014 Msun. However, we
cannot draw any conclusions on cosmological models at this point since
we lack results from realistic numerical simulations containing baryons
to make a proper comparison. We advocate the need for a large sample of
well observed (and well constrained) and simulated unimodal relaxed
galaxy clusters in order to make reliable comparisons and to potentially
provide a test of cosmological models.
Appendix A is only available in electronic form at http://www.aanda.org
AB - Properties of dark matter haloes can be probed observationally and
numerically, and comparing both approaches provides ways to constrain
cosmological models. When it comes to the inner part of galaxy cluster
scale haloes, interaction between the baryonic and the dark matter
component is an important issue that is far from being fully understood.
With this work, we aim to initiate a program coupling observational and
numerical studies to probe the inner part of galaxy clusters. In this
article, we apply strong lensing techniques on Abell 1703, a massive
X-ray luminous galaxy cluster at z = 0.28. Our analysis is based on
imaging data from both the space and ground in 8 bands, complemented by
a spectroscopic survey. Abell 1703 is rather circular from the general
shape of its multiply imaged systems and is dominated by a giant
elliptical cD galaxy in its centre. This cluster exhibits a remarkable
bright central ring formed by 4 images at z_spec = 0.888 only 5-13
arcsec away from the cD centre. This unique feature offers a rare
lensing constrain for probing the central mass distribution. The stellar
contribution from the cD galaxy (˜1.25 × 1012
Msun within 30 kpc) is accounted for in our parametric mass
modelling, and the underlying smooth dark matter component distribution
is described using a generalized nfw profile parametrized with a central
logarithmic slope α. The rms of our mass model in the image plane
is equal to 1.4 arcsec. We find that within the range where
observational constraints are present (from 20 kpc to 210 kpc),
α is equal to 1.09+0.05-0.11 (3σ
confidence level). The concentration parameter is equal to
c200 3.5, and the scale radius is constrained to be larger
than the region where observational constraints are available
(rs =730^+15-75 kpc). The 2D mass is equal to {M}
(210 kpc) = 2.4 × 1014 Msun. However, we
cannot draw any conclusions on cosmological models at this point since
we lack results from realistic numerical simulations containing baryons
to make a proper comparison. We advocate the need for a large sample of
well observed (and well constrained) and simulated unimodal relaxed
galaxy clusters in order to make reliable comparisons and to potentially
provide a test of cosmological models.
Appendix A is only available in electronic form at http://www.aanda.org
U2 - 10.1051/0004-6361:200809646
DO - 10.1051/0004-6361:200809646
M3 - Article
SN - 0004-6361
VL - 489
SP - 23
EP - 35
JO - Astronomy & Astrophysics
JF - Astronomy & Astrophysics
ER -