2010
DOI: 10.1111/j.1365-2966.2010.16305.x
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A model for the cosmological evolution of low-frequency radio sources

Abstract: We present a new evolutionary model that describes the population properties of radio sources at frequencies ≲5 GHz, thus complementing the De Zotti et al. model, holding at higher frequencies. We find that simple analytic luminosity evolution is still sufficient to fit the wealth of available data on local luminosity functions, multifrequency source counts and redshift distributions. However, the fit requires a luminosity‐dependent decline of source luminosities at high redshifts, at least for steep‐spectrum … Show more

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Cited by 98 publications
(171 citation statements)
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“…On the other hand, its very simple assumptions on the extrapolation of source spectra at mm wavelengths as well as new data published in the last ten years make it currently not upof-date for more predictions, although it is still very useful for comparisons -even at ν ≥ 100 GHz -after a simple rescaling (see, e.g., Marriage et al 2011). A&A 533, A57 (2011) More recently, the De Zotti et al (2005) and Massardi et al (2010) new cosmological evolution models of radio sources have been able to give successful fits to the wealth of new available data on luminosity functions, multi-frequency source counts and also redshift distributions at frequencies > ∼ 5 GHz and < ∼ 5 GHz, respectively. These two models are based on an accurate determination of the epoch-dependent luminosity functions (l.f.) for different source populations, usually separated by the value of the spectral index, α, of the observed emission spectrum at low radio frequencies (1 < ∼ ν < ∼ 5 GHz) by adopting a simple powerlaw approximation, i.e., S (ν) ∝ ν α .…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, its very simple assumptions on the extrapolation of source spectra at mm wavelengths as well as new data published in the last ten years make it currently not upof-date for more predictions, although it is still very useful for comparisons -even at ν ≥ 100 GHz -after a simple rescaling (see, e.g., Marriage et al 2011). A&A 533, A57 (2011) More recently, the De Zotti et al (2005) and Massardi et al (2010) new cosmological evolution models of radio sources have been able to give successful fits to the wealth of new available data on luminosity functions, multi-frequency source counts and also redshift distributions at frequencies > ∼ 5 GHz and < ∼ 5 GHz, respectively. These two models are based on an accurate determination of the epoch-dependent luminosity functions (l.f.) for different source populations, usually separated by the value of the spectral index, α, of the observed emission spectrum at low radio frequencies (1 < ∼ ν < ∼ 5 GHz) by adopting a simple powerlaw approximation, i.e., S (ν) ∝ ν α .…”
Section: Introductionmentioning
confidence: 99%
“…Based on these data, many works can be found in the literature where the authors aim at making, and subsequectly improving, the measurement of the ISW effect through correlations with tracer catalogues: 2MASS (an infrared catalogue out to low redshifts around 0.1, Afshordi et al 2004;Rassat et al 2007;Francis & Peacock 2010b;Dupé et al 2011), HEAO (an X-ray survey at low redshift, with the first positive claim of detection, Boughn & Crittenden 2004), Sloan Digital Sky Survey (SDSS, an optical survey at intermediate redshifts, Fosalba et al 2003;Scranton et al 2003;Fosalba & Gaztañaga 2004;Padmanabhan et al 2005;Cabré et al 2006;Giannantonio et al 2006;Granett et al 2009;Xia 2009;Bielby et al 2010;López-Corredoira et al 2010;Sawangwit et al 2010), the NRAO VLA Sky Survey (NVSS, a radio catalogue with high-redshift sources, Boughn & Crittenden 2005;Vielva et al 2006;Pietrobon et al 2006a;McEwen et al 2007;Raccanelli et al 2008;Hernández-Monteagudo 2010;Massardi et al 2010;Schiavon et al 2012), and combined measurements with multiple tracers (Nolta et al 2004;Ho et al 2008;Corasaniti et al 2005;Gaztañaga et al 2006;Giannantonio et al 2008Giannantonio et al , 2012. The significance of the ISW detections that can be found in the literature range between 0.9σ and 4.7σ.…”
Section: Introductionmentioning
confidence: 99%
“…The most recent estimates on source number counts up to ∼50−70 GHz, and the optical identifications of the corresponding bright point sources (see, e.g., Massardi et al 2008Massardi et al , 2010, show that these counts are dominated by radio sources whose average spectral index is "flat", i.e., α 0.0 (with the usual convention S ν ∝ ν α ). This result confirms that the underlying source population is essentially made of flat spectrum radio quasars (FSRQ) and BL Lac objects, collectively called blazars 3 , with minor contributions coming from other source populations (Toffolatti et al 1998;de Zotti et al 2005).…”
Section: Introductionmentioning
confidence: 99%