4.7 Article

The SWELLS survey - II. Breaking the disc-halo degeneracy in the spiral galaxy gravitational lens SDSS J2141-0001

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 417, Issue 3, Pages 1621-1642

Publisher

WILEY-BLACKWELL
DOI: 10.1111/j.1365-2966.2011.18706.x

Keywords

gravitational lensing: strong; galaxies: fundamental parameters; galaxies: haloes; galaxies: kinematics and dynamics; galaxies: spiral; galaxies: structure

Funding

  1. CITA
  2. National Science Foundation Science and Technology Center CfAO [AST-9876783]
  3. NSF [AST 08-08133, NSF-0642621, PHY99-07949]
  4. HST [AR-10664.01-A, HST AR-10965.02-A, HST GO-11206.02-A]
  5. TABASGO foundation
  6. Kavli foundation
  7. Sloan Foundation
  8. NWO-VIDI [639.042.505]
  9. NASA [GO-10587, GO-11978, NAS 5-26555]
  10. W. M. Keck Foundation
  11. Alfred P. Sloan Foundation
  12. Direct For Mathematical & Physical Scien
  13. Division Of Astronomical Sciences [808133] Funding Source: National Science Foundation
  14. Science and Technology Facilities Council [ST/H00243X/1] Funding Source: researchfish

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The degeneracy among the disc, bulge and halo contributions to galaxy rotation curves prevents an understanding of the distribution of baryons and dark matter in disc galaxies. In an attempt to break this degeneracy, we present an analysis of the strong gravitational lens SDSS J2141-0001, discovered as part of the Sloan Lens ACS survey. The lens galaxy is a high-inclination, disc-dominated system. We present new Hubble Space Telescope multicolour imaging, gas and stellar kinematics data derived from long-slit spectroscopy and K-band laser guide star adaptive optics imaging, both from the Keck telescopes. We model the galaxy as a sum of concentric axisymmetric bulge, disc and halo components and infer the contribution of each component, using information from gravitational lensing and gas kinematics. This analysis yields a best-fitting total (disc plus bulge) stellar mass of log(10)(M*/M-circle dot) = 10.99(-0.25)(+ 0.11). The photometric data combined with stellar population synthesis models yield log(10)(M*/M-circle dot) = 10.97 +/- 0.07 and 11.21 +/- 0.07 for the Chabrier and Salpeter initial mass functions (IMFs), respectively. Assuming no cold gas, a Salpeter IMF is marginally disfavoured, with a Bayes factor of 2.7. Accounting for the expected gas fraction of similar or equal to 20 per cent reduces the lensing plus kinematics stellar mass by 0.10 +/- 0.05 dex, resulting in a Bayes factor of 11.9 in favour of a Chabrier IMF. The dark matter halo is roughly spherical, with minor to major axis ratio q(3,h) = 0.91(-0.13)(+0.15). The dark matter halo has a maximum circular velocity of V-max = 276(-18)(+17) km s(-1), and a central density parameter of log(10)Delta(V/2) = 5.9(-0.5)(+0.9). This is higher than predicted for uncontracted dark matter haloes in Lambda cold dark matter cosmologies, log(10)Delta(V/2) = 5.2, suggesting that either the halo has contracted in response to galaxy formation, or that the halo has a higher than average concentration. Larger samples of spiral galaxy strong gravitational lenses are needed in order to distinguish between these two possibilities. At 2.2 disc scalelengths the dark matter fraction is f(DM) = 0.55(-0.15)(+0.20), suggesting that SDSS J2141-0001 is submaximal.

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