Published July 10, 2017 | Version v1
Journal article

Core or Cusps: The Central Dark Matter Profile of a Strong Lensing Cluster with a Bright Central Image at Redshift 1

  • 1. Institute of Cosmology and Gravitation, University of Portsmouth, Portsmouth PO1 3FX (United Kingdom)
  • 2. Fermi National Accelerator Laboratory, P.O. Box 500, Batavia, IL 60510 (United States)
  • 3. Department of Physics, ETH Zurich, Wolfgang-Pauli-Strasse 16, CH-8093 Zurich (Switzerland)
  • 4. Kavli IPMU (WPI), UTIAS, The University of Tokyo, Kashiwa, Chiba 277-8583 (Japan)
  • 5. George P. and Cynthia Woods Mitchell Institute for Fundamental Physics and Astronomy, and Department of Physics and Astronomy, Texas A and M University, College Station, TX 77843 (United States)
  • 6. Department of Physics and Astronomy, Pevensey Building, University of Sussex, Brighton BN1 9QH (United Kingdom)
  • 7. Jodrell Bank Center for Astrophysics, School of Physics and Astronomy, University of Manchester, Oxford Road, Manchester M13 9PL (United Kingdom)
  • 8. Cerro Tololo Inter-American Observatory, National Optical Astronomy Observatory, Casilla 603, La Serena (Chile)
  • 9. CNRS, UMR 7095, Institut d'Astrophysique de Paris, F-75014, Paris (France)
  • 10. Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT (United Kingdom)
  • 11. Kavli Institute for Particle Astrophysics and Cosmology, P.O. Box 2450, Stanford University, Stanford, CA 94305 (United States)

Description

We report on SPT-CLJ2011-5228, a giant system of arcs created by a cluster at z = 1.06. The arc system is notable for the presence of a bright central image. The source is a Lyman break galaxy at z s = 2.39 and the mass enclosed within the Einstein ring of radius 14 arcsec is 10 14.2   M . We perform a full reconstruction of the light profile of the lensed images to precisely infer the parameters of the mass distribution. The brightness of the central image demands that the central total density profile of the lens be shallow. By fitting the dark matter as a generalized Navarro–Frenk–White profile—with a free parameter for the inner density slope—we find that the break radius is 270 76 + 48 kpc, and that the inner density falls with radius to the power −0.38 ± 0.04 at 68% confidence. Such a shallow profile is in strong tension with our understanding of relaxed cold dark matter halos; dark matter-only simulations predict that the inner density should fall as r 1 . The tension can be alleviated if this cluster is in fact a merger; a two-halo model can also reconstruct the data, with both clumps (density varying as r 0.8 and r 1.0 ) much more consistent with predictions from dark matter-only simulations. At the resolution of our Dark Energy Survey imaging, we are unable to choose between these two models, but we make predictions for forthcoming Hubble Space Telescope imaging that will decisively distinguish between them.

Availability note (English)

Available from http://dx.doi.org/10.3847/1538-4357/aa76e6

Additional details

Identifiers

Publishing Information

Journal Title
Astrophysical Journal
Journal Volume
843
Journal Issue
2
Journal Page Range
[13 p.]
ISSN
0004-637X
CODEN
ASJOAB

INIS

Country of Publication
United States
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
51038147
Subject category
S79: ASTROPHYSICS, COSMOLOGY AND ASTRONOMY;
Descriptors DEI
BRIGHTNESS; COMPUTERIZED SIMULATION; DENSITY; FORECASTING; GALAXIES; GALAXY CLUSTERS; GRAVITATIONAL LENSES; MASS; MASS DISTRIBUTION; NONLUMINOUS MATTER; RED SHIFT; RESOLUTION; SPACE; TELESCOPES
Descriptors DEC
DISTRIBUTION; LENSES; MATTER; OPTICAL PROPERTIES; PHYSICAL PROPERTIES; SIMULATION; SPATIAL DISTRIBUTION