Detection of a dark substructure through gravitational imaging
Article first published online: 12 OCT 2010
DOI: 10.1111/j.1365-2966.2010.16865.x
© 2010 The Authors. Journal compilation © 2010 RAS
Issue

Monthly Notices of the Royal Astronomical Society
Volume 408, Issue 4, pages 1969–1981, November 2010
Additional Information
How to Cite
Vegetti, S., Koopmans, L. V. E., Bolton, A., Treu, T. and Gavazzi, R. (2010), Detection of a dark substructure through gravitational imaging. Monthly Notices of the Royal Astronomical Society, 408: 1969–1981. doi: 10.1111/j.1365-2966.2010.16865.x
Publication History
- Issue published online: 28 OCT 2010
- Article first published online: 12 OCT 2010
- Accepted 2010 April 16. Received 2010 March 24; in original form 2009 October 13
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Keywords:
- gravitational lensing: strong;
- galaxies: structure
ABSTRACT
We report the detection of a dark substructure – undetected in the Hubble Space Telescope HST ACS F814W image – in the gravitational lens galaxy SDSSJ0946+1006 (the ‘double Einstein ring’), through direct gravitational imaging. The detection of a small mass concentration in the surface density maps, at 4.3 kpc from the galaxy centre, has a strong statistical significance. We confirm this detection by modelling the substructure with a tidally truncated pseudo-Jaffe density profile; in that case the substructure mass is Msub= (3.51 ± 0.15) × 109 M⊙, precisely where also the surface density map shows a strong convergence peak (Bayes factor
; equivalent to a ∼16σ detection). The result is robust under substantial changes in the model. We set a lower limit of (M/L)V,⊙≳ 120 M⊙/LV,⊙ (3σ) inside a sphere of 0.3 kpc centred on the substructure (rtidal= 1.1 kpc). The mass and luminosity limit of this substructure are consistent with Local Group results if the substructure had a virial mass of ∼1010 M⊙ before accretion and formed at z≳ 10. Our detection implies a projected dark matter mass fraction in substructure at the radius of the inner Einstein ring of f= 2.15+2.05−1.25 per cent [68 per cent confidence level (CL)] in the mass range 4 × 106– 4 × 109 M⊙, assuming α= 1.9 ± 0.1 (with dN/dm∝m−α). Assuming a flat prior on α, between 1.0 and 3.0, increases this to f= 2.56+3.26−1.50 per cent (68 per cent CL). The likelihood ratio is ∼0.5 between these fractions and that from simulations (fN-body≈ 0.003). Hence the inferred dark matter mass fraction in substructure, admittedly based on a single-lens system, is large but still consistent with predictions.

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