First results from the Very Small Array — III. The cosmic microwave background power spectrum

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 341:4 (2003) 1076-1083

Authors:

Paul F Scott, Pedro Carreira, Kieran Cleary, Rod D Davies, Richard J Davis, Clive Dickinson, Keith Grainge, Carlos M Gutiérrez, Michael P Hobson, Michael E Jones, Rüdiger Kneissl, Anthony Lasenby, Klaus Maisinger, Guy G Pooley, Rafael Rebolo, José Alberto Rubiño-Martin, Pedro J Sosa Molina, Ben Rusholme, Richard DE Saunders, Richard Savage, Anže Slosar, Angela C Taylor, David Titterington, Elizabeth Waldram, Robert A Watson, Althea Wilkinson

First results from the Very Small Array — IV. Cosmological parameter estimation

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 341:4 (2003) 1084-1092

Authors:

José Alberto Rubiño-Martin, Rafael Rebolo, Pedro Carreira, Kieran Cleary, Rod D Davies, Richard J Davis, Clive Dickinson, Keith Grainge, Carlos M Gutiérrez, Michael P Hobson, Michael E Jones, Rüdiger Kneissl, Anthony Lasenby, Klaus Maisinger, Carolina Ödman, Guy G Pooley, Pedro J Sosa Molina, Ben Rusholme, Richard DE Saunders, Richard Savage, Paul F Scott, Anže Slosar, Angela C Taylor, David Titterington, Elizabeth Waldram, Robert A Watson, Althea Wilkinson

The cosmic microwave background power spectrum out to ℓ= 1400 measured by the Very Small Array

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 341:4 (2003) l23-l28

Authors:

Keith Grainge, Pedro Carreira, Kieran Cleary, Rod D Davies, Richard J Davis, Clive Dickinson, Ricardo Genova-Santos, Carlos M Gutiérrez, Yaser A Hafez, Michael P Hobson, Michael E Jones, Rüdiger Kneissl, Katy Lancaster, Anthony Lasenby, JP Leahy, Klaus Maisinger, Guy G Pooley, Rafael Rebolo, José Alberto Rubiño-Martin, Pedro J Sosa Molina, Carolina Ödman, Ben Rusholme, Richard DE Saunders, Richard Savage, Paul F Scott, Anže Slosar, Angela C Taylor, David Titterington, Elizabeth Waldram, Robert A Watson, Althea Wilkinson

The Stellar Content of the Bulge of M31**Based on observations with the NASA/ESA Hubble Space Telescope, obtained at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., for NASA under contract NAS 5-26555.

The Astronomical Journal American Astronomical Society 125:5 (2003) 2473-2493

Authors:

Andrew W Stephens, Jay A Frogel, DL DePoy, Wendy Freedman, Carme Gallart, Pascale Jablonka, Alvio Renzini, R Michael Rich, Roger Davies

Emission line widths and QSO black hole mass estimates from the 2dF QSO Redshift Survey

ArXiv astro-ph/0304541 (2003)

Authors:

EA Corbett, SM Croom, BJ Boyle, H Netzer, L Miller, PJ Outram, T Shanks, RJ Smith, K Rhook

Abstract:

We have used composite spectra generated from more than 22000 QSOs observed in the course of the 2dF and 6dF QSO Redshift Surveys to investigate the relationship between the velocity width of emission lines and QSO luminosity. We find that the velocity width of the broad emission lines Hbeta, Hgamma, MgII, CIII] and CIV are correlated with the continuum luminosity, with a significance of more than 99 per cent. Of the major narrow emission lines ([OIII] 5007, [OII] 3727, NeIII 3870 and NeV 3426) only [OIII] exhibits a significant correlation between line width and luminosity. Assuming that the gas is moving in Keplerian orbits and that the radius of the broad line region is related to the QSO continuum luminosity, we use the velocity widths of the broad lines to derive average black hole masses for the QSOs contributing to the composite spectra. The resultant QSO mass-luminosity relationship is consistent with M ~ L^0.97+-0.16. We find that the correlation between line width and redshift, if present, must be weak, and only CIV shows significant evidence of evolution. This enables us to constrain the redshift evolution of the black hole mass-luminosity ratio to be ~(1+z)^beta with beta ~< 1, much less than the ~(1+z)^3 evolution seen in QSO luminosity evolution. Assuming that the motion of the broad line region gas is Keplerian and that its radius depends on the QSO luminosity, our models indicate that the observed weak redshift dependence is too small for the observed QSO luminosity function to be due to the evolution of a single long-lived population of sources.