4.7 Article

The Atacama Cosmology Telescope: measuring radio galaxy bias through cross-correlation with lensing

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 451, Issue 1, Pages 849-858

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stv991

Keywords

large-scale structure of Universe-radio continuum: galaxies

Funding

  1. STFC PhD studentship
  2. US National Science Foundation [AST-0408698, AST-0965625, PHY-0855887, PHY-1214379]
  3. Princeton University
  4. University of Pennsylvania
  5. Cornell University
  6. Canada Foundation for Innovation (CFI)
  7. Comision Nacional de Investigacion Cientifica y Tecnologica de Chile (CONICYT)
  8. CFI under Compute Canada
  9. Government of Ontario
  10. Ontario Research Fund
  11. University of Toronto
  12. NASA [NNX13AE56G, NNX14AB58G]
  13. ERC [259505]
  14. CONICYT [QUIMAL-120001, FONDECYT-1141113]
  15. Misrahi research fund
  16. Wilkinson research fund
  17. Science and Technology Facilities Council [ST/K00106X/1] Funding Source: researchfish
  18. STFC [ST/K00106X/1] Funding Source: UKRI
  19. Division Of Astronomical Sciences
  20. Direct For Mathematical & Physical Scien [1312380, 1440226, 0965625] Funding Source: National Science Foundation

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We correlate the positions of radio galaxies in the FIRST survey with the cosmic microwave background lensing convergence estimated from the Atacama Cosmology Telescope over 470 deg(2) to determine the bias of these galaxies. We remove optically cross-matched sources below redshift z = 0.2 to preferentially select active galactic nuclei (AGN). We measure the angular cross-power spectrum C-t(kg) at 4.4 sigma significance in the multipole range 100 < 1 < 3000, corresponding to physical scales within approximate to 2-60 Mpc at an effective redshift z(eff) = 1.5. Modelling the AGN population with a redshift-dependent bias, the cross-spectrum is well fitted by the Planck best-fitting A cold dark matter cosmological model. Fixing the cosmology and assumed redshift distribution of sources, we fit for the overall bias model normalization, finding b(z(eff)) = 3.5 +/- 0.8 for the full galaxy sample and b(z(eff)) = 4.0 +/- 1.1(3.0 +/- 1.1) for sources brighter (fainter) than 2.5 mJy. This measurement characterizes the typical halo mass of radio-loud AGN: we find log (M-halo/M-circle dot) = 13.6(-0.4)(+0.3).

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