2002
DOI: 10.1046/j.1365-8711.2000.03801.x
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On the redshift cut-off for flat-spectrum radio sources

Abstract: The definitive version is available at www.blackwell-synergy.com Copyright Blackwell Publishing DOI : 10.1046/j.1365-8711.2000.03801.

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Cited by 68 publications
(124 citation statements)
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References 67 publications
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“…Since, on average, these are also the sources with the highest redshifts, this explains our relatively large error bars at z k 2. These results, however, are consistent, for example, with those of Dunlop & Peacock (1990) Jarvis & Rawlings (2000) and Arshakian et al (2006). Stronger evidence for a redshift cutoff comes from the evolution of the FSRQ luminosity function (x 6.2).…”
Section: Evolutionsupporting
confidence: 86%
“…Since, on average, these are also the sources with the highest redshifts, this explains our relatively large error bars at z k 2. These results, however, are consistent, for example, with those of Dunlop & Peacock (1990) Jarvis & Rawlings (2000) and Arshakian et al (2006). Stronger evidence for a redshift cutoff comes from the evolution of the FSRQ luminosity function (x 6.2).…”
Section: Evolutionsupporting
confidence: 86%
“…Such enhancement could indeed be triggered by the radio jets in gas-rich galaxies; however, there are very few radio galaxies at z > 5 (e.g. Jarvis & Rawlings 2000;Jarvis et al 2001a;Wall et al 2005;Rigby et al 2011Rigby et al , 2015. Therefore, it is important to understand at which epochs and under which conditions radio jets can efficiently boost the host galaxy star formation.…”
Section: The Dependence Of Star Formation On Radio Jetsmentioning
confidence: 99%
“…Dunlop & Peacock, 1990). However Jarvis & Rawlings (2000) and Jarvis et al (2001c) highlighted how uncertain the form of this decline is for both flat-spectrum radio-loud quasars (which, crudely speaking, should reflect the overall evolution as it picks out favourably oriented sources from the underlying population) and also low-frequency-selected radio galaxies, due predominantly to difficulties in modelling the k−corrections, and the lack of available volume (and hence small numbers of sources) at high redshift for a given fluxdensity-limited sample. This uncertainty is also mirrored by the X-ray luminosity function (e.g.…”
Section: The High-luminosity Rlf: Friismentioning
confidence: 99%